Medical devices and methods for treatment of hypertension that utilize impedance compensation

ABSTRACT

Medical devices and methods for making and using the same are disclosed. An example medical device may include a control unit for determining an electrical leakage between a first electrode pad and a second electrode pad of an in vivo medical device. The first electrode pad may be spaced from the second electrode pad. The first electrode pad may have an active electrode and a spaced ground electrode. The second electrode pad may have an active electrode and a ground electrode. The ground electrode of the first electrode pad may be electrically connected to the ground electrode of the second electrode pad.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority under 35 U.S.C. §119 to U.S. Provisional Application Ser. No. 61/788,429, filed Mar. 15, 2013, the entirety of which is incorporated herein by reference.

TECHNICAL FIELD

The present disclosure pertains to medical devices, and methods for manufacturing medical devices. More particularly, the present disclosure pertains to medical devices and methods for treatment of hypertension.

BACKGROUND

A wide variety of intracorporeal medical devices have been developed for medical use, for example, intravascular use. Some of these devices include guidewires, catheters, and the like. These devices are manufactured by any one of a variety of different manufacturing methods and may be used according to any one of a variety of methods. Of the known medical devices and methods, each has certain advantages and disadvantages. There is an ongoing need to provide alternative medical devices as well as alternative methods for manufacturing and using medical devices.

BRIEF SUMMARY

Medical devices and methods for making and using medical devices are disclosed.

A control unit for determining an electrical leakage between a first electrode pad and a second electrode pad of an in vivo medical device is disclosed. The first electrode pad may be spaced from the second electrode pad. The first electrode pad may have an active electrode and a spaced ground electrode. The second electrode pad may have an active electrode and a ground electrode. The ground electrode of the first electrode pad may be electrically connected to the ground electrode of the second electrode pad. The control unit may include an input/output block for electrically connecting the control unit to the in vivo medical device and a controller communicatively coupled to the input/output block. The controller may be programmed to apply a first signal via the input/output block to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad. The controller may also be programmed to apply a second signal via the input/output block to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad. In addition, the controller may be programmed to use the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.

Also disclosed are methods for determining an electrical leakage between a first electrode pad and a second electrode pad of an in vivo medical device, where the first electrode pad is spaced from the second electrode pad, and where the first electrode pad has an active electrode and a spaced ground electrode, and the second electrode pad has an active electrode and a ground electrode, where the ground electrode of the first electrode pad is electrically connected to the ground electrode of the second electrode pad. The methods may include applying a first signal to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad. The method may also include applying a second signal to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad. In addition, the method may include using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad. Furthermore, the method may include compensating the measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad based on the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.

A system is also disclosed that may include an in vivo medical device having a first electrode pad and a second electrode pad. The first electrode pad may be spaced from the second electrode pad. The first electrode pad may have an active electrode and a spaced ground electrode. The second electrode pad may have an active electrode and a ground electrode. The ground electrode of the first electrode pad may be electrically connected to the ground electrode of the second electrode pad. A control unit may be coupled to the in vivo medical device. The control unit may be programmed to apply a first signal to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad. The control unit may also be programmed to apply a second signal to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad. The control unit may also be programmed to use the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad and compensate the measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad based on the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.

A method for measuring impedance of a portion of a substance is also disclosed. The method may include bringing at least a portion of an electrode assembly into contact with the substance. The electrode assembly may include a first pair of bipolar electrodes including a first active electrode and a first ground electrode, and a second pair of bipolar electrodes including a second active electrode and a second ground electrode. The first and second ground electrodes may have a common ground. The method may also include measuring impedance between the first active electrode and ground to determine a first measured impedance. The first measured impedance may include a target impedance between the first active electrode and first ground electrode and a leakage impedance between the first active electrode and the second ground electrode. The target impedance and the leakage impedance may be related according to the equation:

(1/M ₁)=(1/Z ₁)+(1/Z ₁₂)

wherein M₁ is the first measured impedance, Z₁ is the target impedance, and Z₁₂ is the leakage impedance.

The method may also include measuring impedance between the second active electrode and ground to determine a second measured impedance. The leakage impedance may be substantially equal to a constant multiplied by the second measured impedance. The method may also include calculating the target impedance using the first measured impedance and the second measured impedance.

Another example method for compensating for an impedance measurement may include providing an electrode assembly including a first electrode pad including a first pair of bipolar electrodes, a second electrode pad including a second pair of bipolar electrodes, and a common ground that is coupled to both the first electrode pad and the first electrode pad. The method may include measuring impedance with the first electrode pad to determine a first measured impedance. The first measured impedance may include a target impedance and a leakage impedance. The target impedance and the leakage impedance may be related according to the formula:

(1/M ₁)=(1/Z ₁)+(1/Z ₁₂)

wherein M₁ is the first measured impedance, Z₁ is the target impedance, and Z₁₂ is the leakage impedance;

The method may also include measuring impedance with the second electrode pad to determine a second measured impedance. The leakage impedance may be substantially equal to a constant multiplied by the second measured impedance. The method may also include calculating the target impedance using the first measured impedance and the second measured impedance.

The above summary of some embodiments is not intended to describe each disclosed embodiment or every implementation of the present disclosure. The Figures, and Detailed Description, which follow, more particularly exemplify these embodiments.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A shows a simplified schematic of an example system for remodeling tissue.

FIG. 1B is a perspective view of an example expandable device of a catheter.

FIG. 1C is a top view of the expandable device of FIG. 1B in an unrolled configuration.

FIGS. 1D and 1E are perspective views of example expandable devices.

FIG. 1F is a perspective view of an example expandable device.

FIG. 2A is a top view of an example electrode assembly.

FIG. 2B is partial cross-sectional view A-A of FIG. 2A.

FIG. 2C is partial cross-sectional view B-B of FIG. 2A.

FIGS. 3A-3D are top views of various example electrode assemblies having multiple electrode pads.

FIGS. 4A-4C are top views of various example electrode assemblies having single distal electrode pads.

FIGS. 5A-5F are top views of various example electrode assemblies having single proximal electrode pads.

FIGS. 5G-I are top views of various example monopolar electrode assemblies.

FIG. 6 is a cross-sectional view of the system of FIG. 1A being used to remodel a body passageway.

FIGS. 7-10 illustrate various, non-limiting, examples of temperature profiles.

FIGS. 11 and 12 illustrate experimental results from a comparison of certain, non-limiting, examples of temperature profiles.

FIGS. 13 and 14 illustrate one embodiment of a control loop.

FIG. 13A illustrates another embodiment of a control loop.

FIG. 15 shows one non-limiting example of a change in temperature over time for an electrode.

FIGS. 16-23 shows one non-limiting example of various attributes associated with eight electrodes during a treatment.

FIGS. 24A-24F are example screen shots from one embodiment of a treatment.

FIGS. 25-30 illustrate one experiment assessing efficacy and safety of an example system for renal denervation.

FIGS. 31 and 32 schematically illustrate example treatment zones associated with two electrodes.

FIG. 33 shows an expandable balloon including an electrode array positioned in a body passageway.

FIGS. 34-38 illustrate an experiment assessing, among other things, the extent of treatment zones created by electro-surgical procedures in tissues proximate renal arteries.

FIGS. 39-41 illustrate an example of overlapping treatment zones during the course of an RF treatment.

FIGS. 42 and 43 schematically illustrate expandable device(s) of a catheter that include electrodes for stimulating and measuring nerve signals.

FIGS. 44 and 45 respectively illustrate a nerve response signal pre-treatment and after receiving at least some treatment.

FIG. 46 illustrates an embodiment of an expandable balloon.

FIGS. 47-50B illustrate embodiments of methods of renal denervation treatments.

FIG. 51 is a schematic view of a portion of an example medical device.

FIG. 52 is a schematic view of a portion of an example medical device.

FIG. 53 is a schematic view of an example control unit.

DETAILED DESCRIPTION

For the following defined terms, these definitions shall be applied, unless a different definition is given in the claims or elsewhere in this specification.

All numeric values are herein assumed to be modified by the term “about,” whether or not explicitly indicated. The term “about” generally refers to a range of numbers that one of skill in the art would consider equivalent to the recited value (i.e., having the same function or result). In many instances, the terms “about” may include numbers that are rounded to the nearest significant figure.

The recitation of numerical ranges by endpoints includes all numbers within that range (e.g. 1 to 5 includes 1, 1.5, 2, 2.75, 3, 3.80, 4, and 5).

As used in this specification and the appended claims, the singular forms “a”, “an”, and “the” include plural referents unless the content clearly dictates otherwise. As used in this specification and the appended claims, the term “or” is generally employed in its sense including “and/or” unless the content clearly dictates otherwise.

It is noted that references in the specification to “an embodiment”, “some embodiments”, “other embodiments”, etc., indicate that the embodiment described may include one or more particular features, structures, and/or characteristics. However, such recitations do not necessarily mean that all embodiments include the particular features, structures, and/or characteristics. Additionally, when particular features, structures, and/or characteristics are described in connection with one embodiment, it should be understood that such features, structures, and/or characteristics may also be used connection with other embodiments whether or not explicitly described unless clearly stated to the contrary.

The following detailed description should be read with reference to the drawings in which similar elements in different drawings are numbered the same. The drawings, which are not necessarily to scale, depict illustrative embodiments and are not intended to limit the scope of the invention.

Physicians use catheters to gain access to and affect therapies by altering interior tissues of the body, particularly within or about the lumens of the body such as blood vessels. For example, balloon angioplasty and other catheters often are used to open arteries that have been narrowed due to atherosclerotic disease.

Catheters can be used to perform renal denervation by RF energy treatment in patients with refractory hypertension. This is a relatively new procedure, which has been found to be clinically effective in treating hypertension. In the procedure, RF energy is applied to walls of the renal artery to reduce hyper-activation (which is often the cause of chronic hypertension) of the sympathetic nervous system adjacent to the renal artery. This procedure has been found to be successful in some cases, but also is associated with a significant amount of pain, and existing treatments can be both relatively difficult for the physician to accurately perform and quite time-consuming.

Another condition affecting many patients is Congestive Heart Failure (“CHF”). CHF is a condition which occurs when the heart becomes damaged and blood flow is reduced to the organs of the body. If blood flow decreases sufficiently, kidney function becomes altered, which results in fluid retention, abnormal hormone secretions and increased constriction of blood vessels. These results increase the workload of the heart and further decrease the capacity of the heart to pump blood through the kidneys and circulatory system.

It is believed that progressively decreasing perfusion of the kidneys is a principal non-cardiac cause perpetuating the downward spiral of CHF. For example, as the heart struggles to pump blood, the cardiac output is maintained or decreased and the kidneys conserve fluid and electrolytes to maintain the stroke volume of the heart. The resulting increase in pressure further overloads the cardiac muscle such that the cardiac muscle has to work harder to pump against a higher pressure. The already damaged cardiac muscle is then further stressed and damaged by the increased pressure. In addition to exacerbating heart failure, kidney failure can lead to a downward spiral and further worsening kidney function. For example, in the forward flow heart failure described above, (systolic heart failure) the kidney becomes ischemic. In backward heart failure (diastolic heart failure), the kidneys become congested vis-a-vis renal vein hypertension. Therefore, the kidney can contribute to its own worsening failure.

The functions of the kidneys can be summarized under three broad categories: filtering blood and excreting waste products generated by the body's metabolism; regulating salt, water, electrolyte and acid-base balance; and secreting hormones to maintain vital organ blood flow. Without properly functioning kidneys, a patient will suffer water retention, reduced urine flow and an accumulation of waste toxins in the blood and body. These conditions result from reduced renal function or renal failure (kidney failure) and are believed to increase the workload of the heart. In a CHF patient, renal failure will cause the heart to further deteriorate as fluids are retained and blood toxins accumulate due to the poorly functioning kidneys. The resulting hypertension also has dramatic influence on the progression of cerebrovascular disease and stroke.

The autonomic nervous system is a network of nerves that affect almost every organ and physiologic system to a variable degree. Generally, the system is composed of sympathetic and parasympathetic nerves. For example, the sympathetic nerves to the kidney traverse the sympathetic chain along the spine and synapse within the ganglia of the chain or within the celiac ganglia, then proceeding to innervate the kidney via post-ganglionic fibers inside the “renal nerves”. Within the renal nerves, which travel along the renal hila (artery and to some extent the vein), are the post-ganglionic sympathetic nerves and the afferent nerves from the kidney. The afferent nerves from the kidney travel within the dorsal root (if they are pain fibers) and into the anterior root if they are sensory fibers, then into the spinal cord and ultimately to specialized regions of the brain. The afferent nerves, baroreceptors and chemoreceptors, deliver information from the kidneys back to the sympathetic nervous system via the brain; their ablation or inhibition is at least partially responsible for the improvement seen in blood pressure after renal nerve ablation, or denervation, or partial disruption. It has also been suggested and partially proven experimentally that the baroreceptor response at the level of the carotid sinus is mediated by the renal artery afferent nerves such that loss of the renal artery afferent nerve response blunts the response of the carotid baroreceptors to changes in arterial blood pressure (American J. Physiology and Renal Physiology 279:F491-F501, 2000, the disclosure of which is incorporated herein by reference).

It has been established in animal models that the heart failure condition results in abnormally high sympathetic activation of the kidneys. An increase in renal sympathetic nerve activity leads to decreased removal of water and sodium from the body, as well as increased renin secretion which stimulates aldosterone secretion from the adrenal gland. Increased renin secretion can lead to an increase in angiotensin II levels, which leads to vasoconstriction of blood vessels supplying the kidneys as well as systemic vasoconstriction, all of which lead to a decrease in renal blood flow and hypertension. Reduction in sympathetic renal nerve activity, e.g., via de-innervation, may reverse these processes and in fact has been shown to in the clinic.

As with hypertension, sympathetic nerve overdrive contributes to the development and progression of CHF. Norepinephrine spillover from the kidney and heart to the venous plasma is even higher in CHF patients compared to those with essential hypertension. Chronic sympathetic nerve stimulation overworks the heart, both directly as the heart increases its output and indirectly as a constricted vasculature presents a higher resistance for the heart to pump against. As the heart strains to pump more blood, left ventricular mass increases and cardiac remodeling occurs. Cardiac remodeling results in a heterogeneous sympathetic activation of the heart which further disrupts the synchrony of the heart contraction. Thus, remodeling initially helps increase the pumping of the heart but ultimately diminishes the efficiency of the heart. Decrease in function of the left ventricle further activates the sympathetic nervous system and the renin-angiotensin-aldosterone system, driving the vicious cycle that leads from hypertension to CHF.

Embodiments of the present disclosure relate to a power generating and control apparatus, often for the treatment of targeted tissue in order to achieve a therapeutic effect. In some embodiments, the target tissue is tissue containing or proximate to nerves, including renal arteries and associated renal nerves. In other embodiments the target tissue is luminal tissue, which may further comprise diseased tissue such as that found in arterial disease.

In yet another exemplary embodiment of the present disclosure, the ability to deliver energy in a targeted dosage may be used for nerve tissue in order to achieve beneficial biologic responses. For example, chronic pain, urologic dysfunction, hypertension, and a wide variety of other persistent conditions are known to be affected through the operation of nervous tissue. For example, it is known that chronic hypertension that may not be responsive to medication may be improved or eliminated by disabling excessive nerve activity proximate to the renal arteries. It is also known that nervous tissue does not naturally possess regenerative characteristics. Therefore it may be possible to beneficially affect excessive nerve activity by disrupting the conductive pathway of the nervous tissue. When disrupting nerve conductive pathways, it is particularly advantageous to avoid damage to neighboring nerves or organ tissue. The ability to direct and control energy dosage is well-suited to the treatment of nerve tissue. Whether in a heating or ablating energy dosage, the precise control of energy delivery as described and disclosed herein may be directed to the nerve tissue. Moreover, directed application of energy may suffice to target a nerve without the need to be in exact contact, as would be required when using a typical ablation probe. For example, eccentric heating may be applied at a temperature high enough to denature nerve tissue without causing ablation and without requiring the piercing of luminal tissue. However, it may also be desirable to configure the energy delivery surface of the present disclosure to pierce tissue and deliver ablating energy similar to an ablation probe with the exact energy dosage being controlled by a power control and generation apparatus.

In some embodiments, efficacy of the denervation treatment can be assessed by measurement before, during, and/or after the treatment to tailor one or more parameters of the treatment to the particular patient or to identify the need for additional treatments. For instance, a denervation system may include functionality for assessing whether a treatment has caused or is causing a reduction in neural activity in a target or proximate tissue, which may provide feedback for adjusting parameters of the treatment or indicate the necessity for additional treatments.

While the disclosure focuses on the use of the technology in the vasculature, the technology would also be useful for other luminal tissues. Other anatomical structures in which the present disclosure may be used are the esophagus, the oral cavity, the nasopharyngeal cavity, the auditory tube and tympanic cavity, the sinus of the brain, the arterial system, the venous system, the heart, the larynx, the trachea, the bronchus, the stomach, the duodenum, the ileum, the colon, the rectum, the bladder, the ureter, the ejaculatory duct, the vas deferens, the urethra, the uterine cavity, the vaginal canal, and the cervical canal.

System Overview

FIG. 1A shows a system 100 for performing a treatment within a body passageway. The system 100 includes a control unit 110. The control unit 110 can include an RF generator for delivering RF energy to catheter device 120. An exemplary control unit and associated energy delivery methods useable with the embodiments disclosed herein are disclosed in commonly assigned U.S. Pat. App. Pub. No. US 2012/0095461, which is incorporated by reference herein. Further examples useable with the embodiments disclosed herein are disclosed in commonly assigned U.S. Pat. No. 7,742,795 entitled “Tuned RF Energy for Selective Treatment of Atheroma and Other Target Tissues and/or Structures”, U.S. Pat. No. 7,291,146 entitled “Selectable Eccentric Remodeling and/or Ablation of Atherosclerotic Material”, and U.S. Pub. No. 2008/0188912 entitled “System for Inducing Desirable Temperature Effects on Body Tissue”, the full disclosures of which are incorporated herein by reference. In some embodiments, particularly in some embodiments utilizing monopolar energy delivery, the system may also include a ground/common electrode, which may be associated with the catheter device, a separate pad that is electrically coupled to the control unit 110, or otherwise associated with system 100.

In some embodiments, the control unit 110 may include a processor or otherwise be coupled to a processor to control or record treatment. The processor will typically comprise computer hardware and/or software, often including one or more programmable processor units running machine readable program instructions or code for implementing some, or all, of one or more of the embodiments and methods described herein. The code will often be embodied in a tangible media such as a memory (optionally a read only memory, a random access memory, a non-volatile memory, or the like) and/or a recording media (such as a floppy disk, a hard drive, a CD, a DVD, a non-volatile solid-state memory card, or the like). The code and/or associated data and signals may also be transmitted to or from the processor via a network connection (such as a wireless network, an ethernet, an internet, an intranet, or the like), and some or all of the code may also be transmitted between components of a catheter system and within the processor via one or more buses, and appropriate standard or proprietary communications cards, connectors, cables, and the like will often be included in the processor. The processor may often be configured to perform the calculations and signal transmission steps described herein at least in part by programming the processor with the software code, which may be written as a single program, a series of separate subroutines or related programs, or the like. The processor may comprise standard or proprietary digital and/or analog signal processing hardware, software, and/or firmware, and may desirable have sufficient processing power to perform the calculations described herein during treatment of the patient, the processor optionally comprising a personal computer, a notebook computer, a tablet computer, a proprietary processing unit, or a combination thereof. Standard or proprietary input devices (such as a mouse, keyboard, touchscreen, joystick, etc.) and output devices (such as a printer, speakers, display, etc.) associated with modern computer systems may also be included, and processors having a plurality of processing units (or even separate computers) may be employed in a wide range of centralized or distributed data processing architectures.

In some embodiments, control software for the system 100 may use a client-server schema to further enhance system ease of use, flexibility, and reliability. “Clients” are the system control logic; “servers” are the control hardware. A communications manager delivers changes in system conditions to subscribing clients and servers. Clients “know” what the present system condition is, and what command or decision to perform based on a specific change in condition. Servers perform the system function based on client commands. Because the communications manager is a centralized information manager, new system hardware may not require changes to prior existing client-server relationships; new system hardware and its related control logic may then merely become an additional “subscriber” to information managed through the communications manager. This control schema may provide the benefit of having a robust central operating program with base routines that are fixed; no change to base routines may be necessary in order to operate new circuit components designed to operate with the system.

Expandable Device and Electrode Assemblies

Returning to FIG. 1A, the catheter device 120 can include an expandable device 130, which can be a compliant, non-compliant, or semi-compliant balloon. The expandable device 130 includes a plurality of electrode assemblies electrically coupled to the control unit 110. Such electrode assemblies can be electrically configured to be monopolar or bipolar, and further have heat sensing capability.

As shown in FIG. 1B, the electrode assemblies may be arranged on the expandable device 130, shown here in an expanded state, according to a plurality of cylindrical treatment zones A-D. In other embodiments, some of which are described further below, the expandable device 130 or other components of the treatment system may include additional electrode assemblies that are not in a treatment zone or are otherwise not used or configured to deliver a treatment energy.

The treatment zones A-D and associated electrode assemblies 140 a-d are further illustrated in FIG. 1C, which is an “unrolled” depiction of the expandable device 130 of FIG. 1B. In some embodiments, the expandable device is a balloon with a 4 mm diameter and two electrode assemblies 140 a-b. In other embodiments, the expandable device is a balloon with a 5 mm diameter and three electrode assemblies 140 a-c. In some embodiments, the expandable device is a balloon with a 6, 7, or 8 mm diameter and four electrode assemblies 140 a-d, as depicted in FIG. 1B. A 4 mm balloon having two electrode assemblies 140 a,b is shown in FIG. 1D and a 5 mm balloon having three electrode assemblies 140 a-c is shown in FIG. 1E. For any of these configurations, the expandable device may have a working length of about 10 mm to about 100 mm, or about 18 mm to about 25 mm, which is the approximate longitudinal span of all the treatment zones A-D shown in FIGS. 1B and 1C. The electrode assemblies 140 a-d can be attached to a balloon using adhesive.

FIG. 1F schematically illustrates an embodiment of an expandable device that includes an array of monopolar electrodes 190 (although, the electrode arrays illustrated in FIGS. 1B through 1E and other figures may also be used in a monopolar configuration). In some instances, one of the monopolar electrodes 190 on the expandable device may be configured to function as a common or ground electrode for the other electrodes. Alternatively, separate or differently shaped and configured electrodes on the expandable device (such as ring electrode 192 illustrated in broken lines in FIG. 1F) or electrodes on other expandable devices (e.g. 194 in FIG. 1G) or otherwise associated with the catheter may be configured as a common electrode. In still other instances, a grounding pad may be secured to the patient's skin to function as the common electrode. Although not shown explicitly in FIG. 1G, the monopolar electrodes may each be positioned proximate or on a temperature sensing device, similar to other embodiments described herein.

a. Overlapping and Non-Overlapping Treatment Zones

Returning to FIG. 1B, the treatment zones A-D are longitudinally adjacent to one another along longitudinal axis L-L, and may be configured such that energy applied by the electrode assemblies create treatments that do not overlap. Treatments applied by the longitudinally adjacent bipolar electrode assemblies 140 a-d are circumferentially non-continuous along longitudinal axis L-L. For example, with reference to FIG. 1C, lesions created in treatment zone A may in some embodiments minimize overlap about a circumference (laterally with respect to L-L in this view) with lesions created in treatment zone B.

In other embodiments, however, the energy applied by the electrode assemblies, such as the electrode assemblies shown in FIG. 1C, may overlap, longitudinally, circumferentially, and/or in other ways, to at least some extent. FIGS. 31 and 32 schematically illustrate non-limiting examples of how electrodes 3102 and 3104 may be energized to create overlapping treatment zones. Although not shown specifically in FIGS. 31 and 32, electrodes 3102 and 3104 may each be a bipolar electrode pair (or may be single monopolar electrodes), and may be positioned on an outer surface of a catheter balloon or other expandable device such that they are longitudinally and circumferentially offset from one another (e.g. as in FIG. 1C). As shown in FIG. 31, each of electrodes 3102 and 3104 may be associated with a treatment zone (or may be configured to create such a treatment zone in a tissue in apposition with the electrodes) that includes a target temperature zone (the outer boundary of which is labeled “TT”) and a thermal plume (the outer boundary of which is labeled “TP”). In some embodiments, the target temperature zone represents a region of the tissue that is at or above a desired target treatment temperature, or is within a desired target temperature range. In some embodiments, the thermal plume represents a region of the tissue that is not necessarily at a target temperature or within a target temperature range, but exhibits an increase in temperature relative to an untreated zone outside of the thermal plume.

Whether or not treatment zones between electrodes/electrode pairs will overlap may be influenced by a wide variety of factors, including, but not limited to, electrode geometry, electrode placement density, electrode positioning, ground/common electrode(s) placement and geometry (in monopolar embodiments), energy generator output settings, output voltage, output power, duty cycle, output frequency, tissue characteristics, tissue type, etc.

In some embodiments, individual electrodes of a bipolar electrode pair may each define its own treatment zone, and such treatment zones may partially or entirely overlap.

In FIG. 31, the thermal plumes of the treatment zones overlap, although the target temperature zones do not. In FIG. 32, both the target temperature zones and the thermal plumes overlap. In some embodiments, the overlap of treatment zones may extend substantially continuously around a circumference of the device and/or around a circumference in a tissue surrounding a body passageway. In other embodiments, there may be overlap in treatment zones, however, that overlap will not be substantially continuous around a circumference and significant discontinuities in the treatment zones may be present.

It has been experimentally determined that at least some electrosurgical systems utilizing an array of balloon-mounted electrodes can create overlapping treatment zones between adjacent electrode pads, and, in at least some instances, create treatment zones that are effectively substantially continuous about a circumference of a body passageway. In one experiment, a catheter and expandable balloon similar to that shown and described in U.S. Pub. No. 2008/0188912 (incorporated in its entirety by this reference), particularly at FIG. 9C (reproduced here as FIG. 33), was used to generate overlapping treatment zones between adjacent electrode pairs, such that a treatment zone effectively extended substantially continuously about a circumference. As shown in FIG. 33, the expandable balloon 20 includes several longitudinally extending series of bipolar electrode pairs 34 positioned about the circumference of the balloon. Unlike the electrode arrays shown in, for instance, FIG. 1C, the electrode arrays shown in FIG. 33 are arranged symmetrically on the expandable balloon 20.

In one experiment utilizing a catheter-based balloon electrode array similar to that of FIG. 33, local response of fourteen renal vessels that were either treated with various power and duration of radio-frequency regimens (about 60° C. to about 75° C. for about 5 seconds to about 120 seconds), or left untreated, was evaluated on day 28±1 and day 84. Additionally, the kidneys from a total of 7 animals were evaluated via light microscopy.

Kidneys and renal arteries were explanted intact with underlying muscle and fixed in 10% neutral buffered formalin. Fixed tissues were then submitted for histopathological processing and evaluation. Each vessel was trimmed at approximately every 3-4 mm until the tissue was exhausted, processed, embedded in paraffin, sectioned twice at ˜5 microns, and stained with hematoxylin and eosin (H+E) and elastin trichrome (ET). Kidneys were trimmed at three levels (cranial, center and caudal), processed, embedded in paraffin, sectioned and stained with H+E. All resulting slides were examined via light microscopy.

Evaluation of step sections from six acute arteries treated at various power and duration of radio-frequency regimens or left untreated, and evaluation of dependent kidneys showed acute thermal changes characterized by coagulation necrosis in the media and perivascular tissues and collagen hyalinization. FIG. 34 shows a cross section of a left renal artery (labeled A) and surrounding tissue treated with six pairs of electrodes in a 75° C. protocol for ten seconds. In FIG. 34, circumferential thermal injury was observed within the boundaries of the dotted line, including injury to several nerve branches (as indicated by the arrowheads), a ganglion (short arrow) and a portion of the adjacent lymph node (LN). FIG. 35 shows a cross section of a right renal artery and surrounding tissue treated with six pairs of electrodes in a 75° C. protocol for five seconds. In FIG. 35, circumferential injury was observed within the boundaries of the dotted line and includes several nerve branches (as indicated by the arrowheads). Referring to FIGS. 34 and 35, thermal injury was circumferential in the central-most segment treated in the left artery and in the media of the right artery. The kidneys showed no treatment-related changes. Circumferential treatment was effective at reaching and creating injury in extrinsic renal innervation with a radial reach that was up to 10 mm in depth. There was minimal to notable procedural injury caused by balloon treatment of a magnitude likely to trigger a significant restenotic response.

FIGS. 36 and 37 show additional cross sections of the left renal artery of FIG. 34, at day 27 post treatment. FIG. 38 is another representative low magnification image of a 75° C. RF treatment. The zones of treatment in FIG. 38 are evidenced by residual necrotic tunica media and adventitial thickening by early smooth muscle cell hyperplasia, fibroplasia, and inflammatory infiltrates (e.g., brackets). FIG. 38 also shows extension of the zone of treatment into the adjacent adventitia (as shown by the dashed lines).

FIGS. 39-41 further illustrates how, in some embodiments, treatment zones can overlap over the course of an RF energy treatment. FIGS. 39-41 illustrate a Vessix V2 catheter positioned in a cylinder filled with a thermo-sensitive gel over the course of a thirty second treatment. FIG. 39 shows the thermo-sensitive gel just after treatment initiation, with the square shaped patches in the gel indicating localized electrode heating. As shown in FIG. 40, as the treatment progresses, the patches in the gel increase in size due to heat conduction and come close to touching. FIG. 41 shows the gel at the completion of a 30 second treatment, showing substantial overlap in the patches.

b. Electrode Assembly Structure

Returning to FIG. 1C, each electrode pad assembly includes four major elements, which are a distal electrode pad 150 a-d, intermediate tail 160 a-d, proximal electrode pad 170 a-d, and proximal tail 180 b,d (not shown for electrode pad assemblies 140 b and 140 c). Constructional details of the electrode assemblies 140 a-d are shown and described with reference to FIGS. 2A-C.

FIG. 2A shows a top view of electrode assembly 200, which is identified in FIG. 1C as electrode assembly 140. The electrode assembly 200 is constructed as a flexible circuit having a plurality of layers. Such layers can be continuous or non-contiguous, i.e., made up of discrete portions. Shown in FIGS. 2B and 2C, a base layer 202 of insulation provides a foundation for the electrode assembly 200. The base layer 202 can be constructed from a flexible polymer such as polyimide. In some embodiments, the base layer 202 is approximately 0.5 mil (0.0127 mm) thick. A conductive layer 204 made up of a plurality of discrete traces is layered on top of the base layer 202. The conductive layer 204 can be, for example, a layer of electrodeposited copper. In some embodiments, the conductive layer 204 is approximately 0.018 mm thick. An insulating layer 206 is discretely or continuously layered on top of the conductive layer 204, such that the conductive layer 204 is fluidly sealed between the base layer 202 and the insulating layer 206. Like the base layer 202, the insulating layer 206 can be constructed from a flexible polymer such as polyimide. In some embodiments, the insulating layer 206 is approximately 0.5 mil (0.0127 mm) thick. In other embodiments, the insulating layer 206 is a complete or partial polymer coating, such as PTFE or silicone.

The electrode assembly 200 shown in FIG. 2A includes a distal electrode pad 208. In this region, the base layer 202 forms a rectangular shape. As shown, the electrode assembly 200 may include a plurality of openings to provide for added flexibility, and the pads and other portions of the assemblies may include rounded or curved corners, transitions and other portions. In some instances, the openings and rounded/curved features may enhance the assembly's resistance to delamination from its expandable device, as may occur, in some instances, when the expandable device is repeatedly expanded and collapsed (which may also entail deployment from and withdrawal into a protective sheath), such as may be needed when multiple sites are treated during a procedure.

The distal electrode pad 208 includes a plurality of discrete traces layered on top of the base layer 202. These traces include a ground trace 210, an active electrode trace 212, and a sensor trace 214. The ground trace 210 includes an elongated electrode support 216 laterally offset from a sensor ground pad 218. The sensor ground pad 218 is electrically coupled to the elongated support 216 of the ground trace 210 and is centrally located on the distal electrode pad 208. A bridge 220 connects a distal most portion of the sensor ground pad 218 to a distal portion of the elongated electrode support 216 of the ground trace 210. The bridge 220 tapers down in width as it travels to the sensor ground pad 218. In some embodiments, the bridge 220 has a relatively uniform and thin width to enable a desired amount of flexibility. The elongated electrode support 216 tapers down in width at its proximal end, however, this is not required. In some embodiments, the elongated electrode support 216 can abruptly transition to a much thinner trace at its proximal portion, to enable a desired amount of flexibility. Generally, the curvature of the traces where necking is shown is optimized to reduce balloon recapture forces and the potential for any snagging that sharper contours may present. The shape and position of the traces are also optimized to provide dimensional stability to the electrode assembly 200 as a whole, so as to prevent distortion during deployment and use.

The ground trace 210 and active electrode trace 212 of FIG. 2A share a similar construction. The active electrode trace 212 also includes an elongated electrode support 216.

FIG. 2B shows a partial cross-section A-A of the distal electrode pad 208. An electrode 222 is shown layered over a portion of the insulating layer 206, which has a plurality of passages (e.g., holes) to enable the electrode 222 to couple to the elongated electrode support 216 of the ground trace 210 (of conductive layer 204).

As shown in FIG. 2A, the ground electrode trace 210 and active electrode trace 212 can include a plurality of electrodes. Three electrodes 222 are provided for each electrode trace, however, more or less can be used. Additionally, each electrode 222 can have radiused corners to reduce tendency to snag on other devices and/or tissue. Although the above description of the electrodes 222 and the traces associated with them has been described in the context of a bi-polar electrode assembly, those of skill in the art will recognize that the same electrode assembly may function in a monopolar mode as well. For instance, as one non-limiting example, the electrodes associated with active electrode traces 212 and 242 may be used as monopolar electrodes, with ground trace 210 disconnected during energization of those electrodes.

It has been experimentally determined that an example embodiment for a renal hypertension indication having an approximate longitudinal length of 4 mm per plurality of electrodes, including longitudinal spacing between electrodes 222, provides effective tissue remodeling results with respect to optimal lesion size and depth, while avoiding a stenoic response. The shown configuration was arrived at by balancing depth of thermal penetration, and avoidance of thermal damage to tissue collateral the treatment zone, while seeking to minimize the number of electrode pairs to optimize flexibility and profile on a final device However, the shown configuration is not a necessary requirement, since electrode size and placement geometry can vary according to desired therapeutic effect.

Thirty-three Yorkshire swine were subjected to renal denervation (RDN) by Vessix Vascular's renal denervation radiofrequency (RF) balloon catheters. Putative renal denervation through Vessix Vascular's electrode design was accomplished through a spectrum of settings (a function of electrode length, temperature, and duration) to compare the safety at 7 days and 28 days post-procedure between Vessix 16 mm circumferential electrodes vs. 2 mm and 4 mm electrode with offset design. Histologic sections of the renal arteries were examined to evaluate the tissue response including, but not limited to: injury, inflammation, fibrosis, and mineralization at 7 and 28 days.

The treatment of renal arteries with the Vessix Vascular RDN RF Balloon Catheter resulted in a spectrum of changes in the arterial wall and adjacent adventitia, which represented the progression of the arterial/adventitial response from an acute, “injurious” phase to a chronic, “reactive/reparative” phase. Treated areas within the renal arteries were apparent due to the presence of these changes in the arterial wall and extension thereof into the adjacent adventitial tissue (interpreted as the “zone of treatment”).

At Day 7, all electrodes, regardless of length, treatment temperature or duration were associated with a primarily injurious response. However, the 2 mm and 4 mm electrodes were also associated with an early reactive/reparative response, regardless of treatment duration, which was not observed with either 16 mm RF treatment at Day 7. The overall extent of arterial circumference affected with the 16 mm electrodes was increased (mild/moderate to marked, ˜>75% to 100% of circumference covered, respectively), regardless of temperature, relative to the shorter electrodes (2 mm and 4 mm) in which the affect was typically minimal to mild/moderate (˜<25% to ˜25-75% circumference affected, respectively), regardless of duration of treatment.

At Day 28, frequent, minimal neointima formation was observed, regardless of time point, in all treatment groups with the exception of the shorter 4 mm electrode. Mild/moderate neointima formation was infrequently observed only at Day 28, regardless of treatment group; however, the 16 mm electrodes were associated with a mild and comparable increase in the incidences of mild/moderate neointima relative to the shorter 2 and 4 mm electrode.

The denudation (i.e., loss) of endothelial cells is a common sequelae to the passage of any interventional device as well as an expected sequelae to the treatment with the Vessix Vascular RDN RF Balloon Catheter. Due to the importance of the endothelium in preventing thrombus formation, its recovery in denuded regions was monitored. As such, the magnitude/extent of the re-endothelialization of the luminal surface was interpreted relative to the approximate circumference of the artery affected

At Day 7, the 2 and 4 mm electrodes had more arterial sections with complete endothelialization than not; complete endothelialization was present in all arterial sections of the 2 and 4 mm electrode. No arterial section treated with a 16 mm electrode was observed to have complete endothelialization at Day 7, regardless of dose.

At Day 7, inflammation was overall typically minimal, regardless of treatment; however, both 16 mm electrodes, regardless of dose, had an overall increase in inflammation relative to 2 and 4 mm electrodes. Mild/moderate inflammatory infiltrates were rarely observed in the 2 and 4 mm electrode, but were frequent to common in the 16 mm electrodes.

In the embodiment of FIG. 2A, each electrode 222 is approximately 1.14 mm by 0.38 mm, with approximately 0.31 mm gaps lying between the electrodes 222. The electrodes 222 of the ground trace 210 and active electrode trace 212 are laterally spaced by approximately 1.85 mm. In some embodiments, such as the embodiment shown in FIG. 2B, the electrodes 222 are gold pads approximately 0.038 mm thick from the conductive layer 204 and that protrude 0.025 mm above the insulating layer 206. Without limiting the use of other such suitable materials, gold is a good electrode material because it is very biocompatible, radiopaque, and electrically and thermally conductive. In other embodiments, the electrode thickness of the conductive layer 204 can range from about 0.030 mm to about 0.051 mm. At such thicknesses, relative stiffness of the electrodes 222, as compared to, for example, the copper conductive layer 204, can be high. Because of this, using a plurality of electrodes, as opposed to a single electrode, can increase flexibility. In other embodiments, the electrodes may be as small as 0.5 mm by 0.2 mm or as large as 2.2 mm by 0.6 mm for electrode 222.

While it is an important design optimization consideration to balance the thickness of the gold above the insulating layer 206 so as to achieve good flexibility while maintaining sufficient height so as to provide good tissue contact, this is counterbalanced with the goal of avoiding a surface height that may snag during deployment or collapse of the balloon. These issues vary according to other elements of a particular procedure, such as balloon pressure. For many embodiments, it has been determined that electrodes that protrude approximately 0.025 mm above the insulating layer 206 will have good tissue contact at balloon inflation pressures below 10 atm and as low as 2 atm. These pressures are well below the typical inflation pressure of an angioplasty balloon.

The sensor trace 214 is centrally located on the distal electrode pad 208 and includes a sensor power pad 224 facing the sensor ground pad 218. These pads can connect to power and ground poles of a heat sensing device 226, such as a thermocouple (for example, Type T configuration: Copper/Constantan) or thermistor, as shown in the partial cross-section depicted in FIG. 2C.

The heat sensing device 226 is proximately connected to the sensor power pad 224 and distally connected to the sensor ground pad 218. To help reduce overall thickness, the heat sensing device 226 is positioned within an opening within the base layer 202. In some embodiments, the heat sensing device 226 is a thermistor having a thickness of 0.1 mm, which is unusually thin—approximately two-thirds of industry standard. As shown, the heat sensing device 226 is on a non-tissue contacting side of the distal electrode pad 208. Accordingly, the heat sensing device 226 is captured between the electrode structure and a balloon when incorporated into a final device, such as catheter 120. This is advantageous since surface-mounted electrical components, like thermistors, typically have sharp edges and corners, which can get caught on tissue and possibly cause problems in balloon deployment and/or retraction. This arrangement also keeps soldered connections from making contact with blood, since solder is typically non-biocompatible. Further, due to the placement of the heat sensing device, it can measure temperature representative of tissue and the electrodes 222. Designs in the prior art typically take one of two approaches—either contacting tissue or contacting the electrode. Here, neither of these prior approaches are employed.

From the rectangular distal electrode pad 208, the combined base layer 202, conductive layer 204, and insulating layer 206 reduce in lateral width to an intermediate tail 228. Here, the conductive layer 204 is formed to include an intermediate ground line 230, intermediate active electrode line 232, and intermediate sensor line 234, which are respectively coextensive traces of the ground trace 210, active electrode trace 212, and sensor trace 214 of the distal electrode pad 208.

From the intermediate tail 228, the combined base layer 202, conductive layer 204, and insulating layer 206 increase in lateral width to form a proximal electrode pad 236. The proximal electrode pad 236 is constructed similarly to the distal electrode pad 208, with the electrode geometry and heat sensing device arrangement being essentially identical, although various differences may be present. However, as shown, the proximal electrode pad 236 is laterally offset from the distal electrode pad 208 with respect to a central axis G-G extending along the intermediate ground line 230. The intermediate active electrode line 232 and intermediate sensor line 234 are laterally coextensive with the proximal electrode pad 236 on parallel respective axes with respect to central axis G-G.

From the proximal electrode pad 236, the combined base layer 202, conductive layer 204, and insulating layer 206 reduce in lateral width to form a proximal tail 238. The proximal tail 238 includes a proximal ground line 240, proximal active electrode line 242, and proximal sensor line 244, as well the intermediate active electrode line 232 and intermediate sensor line 234. The proximal tail 238 includes connectors (not shown) to enable coupling to one or more sub-wiring harnesses and/or connectors and ultimately to control unit 110. Each of these lines are extended along parallel respective axes with respect to central axis G-G.

As shown, the electrode assembly 200 has an asymmetric arrangement of the distal electrode pad 208 and proximal electrode pad 236, about axis G-G. Further, the ground electrodes of both electrode pads are substantially aligned along axis G-G, along with the intermediate and proximal ground lines 230/240. It has been found that this arrangement presents many advantages. For example, by essentially sharing the same ground trace, the width of the proximal tail is only about one and a half times that of the intermediate tail 228, rather than being approximately twice as wide if each electrode pad had independent ground lines. Thus, the proximal tail 238 is narrower than two of the intermediate tails 228.

Further, arranging the electrode pads to share a ground trace allows control of which electrodes will interact with each other. This is not immediately apparent when viewing a single electrode assembly, but becomes evident when more than one electrode assembly 200 is assembled onto a balloon, for example as shown in FIG. 1C. The various electrode pads can be fired and controlled using solid state relays and multiplexing with a firing time ranging from about 100 microseconds to about 200 milliseconds or about 10 milliseconds to about 50 milliseconds. For practical purposes, the electrode pads appear to be simultaneously firing yet stray current between adjacent electrode pads of different electrode assemblies 200 is prevented by rapid firing of electrodes in micro bursts. This can be performed such that adjacent electrode pads of different electrode pad assemblies 200 are fired out of phase with one another. Thus, the electrode pad arrangement of the electrode assembly allows for short treatment times—10 minutes or less of total electrode firing time, with some approximate treatment times being as short as 10 seconds, with and exemplary embodiment being about 30 seconds. The benefits of short treatment times include minimization of post-operative pain caused when nerve tissue is subject to energy treatment, shortened vessel occlusion times, reduced occlusion side effects, and quick cooling of collateral tissues by blood perfusion due to relatively minor heat input to luminal tissue.

In some embodiments, the common ground typically carries 200 VAC at 500 kHz coming from the negative electrode pole, and a 1V signal from the heat sensing device 226 (in the case of a thermistor) that requires filtering of the RF circuit such that the thermistor signal can be sensed and used for generator control. In some embodiments, because of the common ground, the thermistor of the adjacent electrode pair may be used to monitor temperature even without firing the adjacent electrode pair. This provides the possibility of sensing temperatures proximate to both the distal electrode pad 208 and the proximal electrode pad 236, while firing only one of them.

Referring again to FIG. 1C, the electrode pad arrangement of each electrode assembly 140 a-d also enables efficient placement on balloon 130. As shown, the electrode assemblies 140 a-d “key” into one another to enable maximum use of balloon surface area. This is accomplished in part by spacing the electrode pads apart by setting the longitudinal length of each intermediate tail. For example, the intermediate tail length electrode assembly 140 a is set to a distance that separates its distal and proximal electrode pads 150 a,170 a such that the laterally adjacent proximal electrode pad 170 b of the laterally adjacent electrode assembly 140 b keys next to the intermediate tail 160 a of electrode assembly 140 a. Further, the distal electrode pad 150 a of electrode assembly 140 a is keyed between the intermediate tail 160 b of electrode assembly 140 b and the intermediate tail 160 d of electrode assembly 140 d. Thus, the length of each intermediate tail 160 a-d also requires each electrode pad of any one electrode assembly to be located in non-adjacent treatment zones.

Balloon surface area maximization is also enabled in part by laterally offsetting both electrode pads of each electrode assembly 140 a-d. For example, the rightwards lateral offset of each distal electrode pad 150 a-d and the leftwards lateral offset of the proximal electrode pad 170 a-d allow adjacent electrode pad assemblies to key into one another such that some of the electrode pads laterally overlap one another. For example, the distal electrode pad 150 a of electrode assembly 140 a laterally overlaps with proximal electrode pad 170 b of electrode assembly 140 b. Further, the distal electrode pad 150 b of electrode assembly 140 b laterally overlaps with the proximal electrode pad 170 c of electrode assembly 140 c. However, the length of each intermediate tail prevents circumferential overlap (longitudinal overlap in this view) of the electrode pads, thus maintaining the non-contiguous nature of the treatment zones in the longitudinal direction L-L.

The arrangement and geometry of the electrode pads, as well as the arrangement and geometry of the tails of the flexible circuits may also facilitate folding or otherwise collapsing the balloon into a relatively compact un-expanded state. For instance, in embodiments with an expanded diameter of up to 10 mm, the device in an un-expanded state may have as low as an approximately 1 mm diameter.

Some embodiments utilize a standard electrode assembly having identical dimensions and construction, wherein the number and relative position of electrode assemblies on an outer surface of a balloon becomes a function of balloon diameter and/or length while electrode assembly geometries remain unchanged amongst various balloon sizes. The relative positioning of electrode assemblies relative to balloon diameter and/or length may then be determined by the desired degree or avoidance of circumferential and/or axial overlap of adjacent electrode pads of neighboring electrode assemblies on a balloon of a given size. In other embodiments, however, all of the electrode assemblies on the balloon will not necessarily be identical.

FIGS. 3A-3D shows alternative electrode pad configurations useable with the system 100 of FIG. 1A. FIG. 3A shows an electrode assembly 300 that is constructed similarly to electrode assembly 200, but having two electrode pads 302 that are directly adjacent to one another.

FIG. 3B shows an electrode pad assembly 304 that is constructed similarly to electrode assembly 200, but having two electrode pads 306 that are directly adjacent to one another. Further, the electrode pads 306 have electrodes arranged to be transverse with respect to longitudinal axis L-L of FIGS. 1C and G-G of FIG. 2A.

FIG. 3C shows an electrode assembly 310 that is constructed similarly to electrode assembly 304, but having three staggered and separated electrode pads 312. Like the electrode assembly 304 of FIG. 3B, the electrode pads 312 feature transversely arranged electrodes.

FIG. 3D shows an electrode assembly 314 that is constructed similarly to electrode assembly 310, but having electrode pads 312 with greater electrode surface area. Like the electrode assembly 304 of FIG. 3B, the electrode pads 316 feature transversely arranged electrodes.

FIGS. 4A-4C shows alternative electrode pad configurations useable with the system 100 of FIG. 1A. FIG. 4A shows an electrode assembly 400 that is constructed similarly to electrode assembly 200, but having only a single distal electrode pad 402.

FIG. 4B shows an electrode assembly 404 that is constructed similarly to electrode assembly 400, but having an single distal electrode pad 407 with a greater active electrode 408 surface area than ground surface area 410.

FIG. 4C shows an electrode assembly 412 that is constructed similarly to electrode assembly 404, but having a single distal electrode pad 414 having a heavily porous construction to enable greater flexibility.

FIGS. 5A-5F shows alternative electrode configurations useable with the system 100 of FIG. 1A. In some embodiments, the shown electrode configurations are useable with the configurations of FIGS. 4A-4C. FIG. 5A shows an electrode assembly 500 that is constructed similarly to electrode assembly 400, but arranged to include only a single proximal electrode pad 502. The electrode assembly 500 further includes an elongated distal portion 504 for attachment to a balloon.

FIG. 5B shows an electrode assembly 506 that is constructed similarly to electrode assembly 500, but having more comparative electrode surface area on electrode pad 508.

FIG. 5C shows an electrode assembly 510 that is constructed similarly to electrode assembly 500, but having more comparative electrode surface area on electrode pad 512 and a larger number of electrodes.

FIG. 5D shows an electrode assembly 514 that is constructed similarly to electrode assembly 510, but having a non-uniform electrode configuration on electrode pad 512.

FIG. 5E shows an electrode assembly 514 that is constructed similarly to electrode assembly 500, but having less comparative electrode surface area on electrode pad 516 and a smaller number of electrodes 518. Electrode pad 516 also incorporates two heat sensing devices 520 mounted on the same side as electrodes.

FIG. 5F shows an electrode assembly 522 that is constructed similarly to electrode assembly 514, but having a transversely arranged electrode 524 and a single heat sensing device 526.

The electrode assemblies of FIGS. 2 through 5F may be used in bipolar or monopolar configurations. FIGS. 5G through 5I illustrate additional examples of monopolar electrode configurations. In FIG. 5G there are two parallel arrays of monopolar electrodes 530 on either side of temperature sensor 532. In FIG. 5G, each array of monopolar electrodes 530 has its own discrete trace, with the temperature sensor 532 having its own discrete trace as well. In other embodiments, however, all of the monopolar electrodes 530 on a particular flex circuit assembly may share a single active trace, and one of the temperature sensor's two traces may be shared as well, although, in other embodiments, the power and ground traces for the temperature sensor may be separate from the monopoloar trace(s).

FIG. 5H illustrates another arrangement for a monopolar electrode pad in which all of the monopolar electrodes 536 are coupled to a single trace. FIG. 5I shows another alternative arrangement for the monopolar electrodes and temperature sensor. The monopolar electrode pads may be arranged about an expandable device in longitudinally and circumferentially offset arrangements (such as shown in FIG. 1C) and may have geometries and arrangements similar to those shown in FIGS. 3A through 5F.

Treatment Methods and Control Systems

a. Device Positioning

FIG. 6 shows the system 100 of FIG. 1A being used to perform a method 600 of treatment in accordance with one non-limiting embodiment of the disclosure. Here, control unit 110 is shown operationally coupled to catheter device, which has been placed in a body passageway such that an expandable device (having a plurality of electrode assemblies) is placed adjacent to a section S1 of the body passageway where therapy is required. Placement of the catheter device at section S1 can be performed according to conventional methods, e.g., over a guidewire under fluoroscopic guidance. Once placed in S1, the expandable device can be made to expand, e.g., by pressurizing fluid from 2-10 atm in the case of a balloon. This causes electrodes of the expandable device to come into contact with the body passageway.

In some embodiments, control unit 110 may measure impedance at the electrode assemblies to confirm apposition of the electrodes with the body passageway. In at least some of these embodiments, the treatment may proceed even if apposition is not sensed for all of the electrodes. For instance, in some embodiments, the treatment may proceed if apposition is sensed for 50% or more of the electrodes, and may allow for less than complete uniformity of apposition circumferentially and/or axially. For example, in some instances the catheter may be positioned such that one or more of the proximal electrodes are in the aorta and exposed to blood, and impedance sensed for such electrodes may not fall within a pre-designated range (such as, for example, 500-1600 ohms), indicating an absence of tissue apposition for those electrodes. In some instances, the system may allow for user authorization to proceed with the treatment even if there is less than uniform electrode/tissue apposition. Subsequently, the control unit 110 may activate the electrodes to create a corresponding number of lesions L, as indicated by the black squares. During activation of the electrodes, the control unit uses heat sensing devices of the electrode pads to monitor both heat of the electrode and the tissue due to the unique arrangement of the heat sensing devices, which do not contact either tissue or electrodes. In this manner, more or less power can be supplied to each electrode pad as needed during treatment.

In some embodiments, control unit 110 may apply a uniform standard for determining apposition to all the electrodes of the device. For instance, the control unit may utilize the same pre-designated range of resistance measurements to all of the electrodes. In other instances, however, including some, although not all, monopolar applications, different standards may be applied to different monopolar electrodes for determining apposition. For example, in some monopolar embodiments, each monopolar electrode may define a discrete electrical circuit through the tissue to the common/indifferent electrode (or electrodes), and the characteristics of those circuits (e.g. resistance) may vary significantly based on the distance between the monopolar electrode and common electrode, the tissue characteristics therebetween, and other geometries and characteristics of the device and surrounding tissue. As such, in at least some embodiments, it may be desirable to apply criteria for determining apposition that varies depending on, e.g., the distance between the monopolar electrode and common electrode (e.g. the greater the distance between the two electrodes, the higher the impedance measurement required to determine good apposition). In other embodiments, however, the variance due to these differences in distance and other geometries will be minimal or non-substantive, and a uniform standard may be applied.

FIGS. 24A-F illustrate one non-limiting example of a series of screen shots displayed by the control unit during the course of a treatment. In FIG. 24A, the system prompts a user to connect a catheter. In FIG. 24B, the system confirms that a catheter has been connected and other information about the connected catheter (e.g. size/diameter). At FIGS. 24C and D, the system, as discussed above, can check for electrode apposition, indicate which or what number of electrodes are in apposition, and ask for authorization to proceed. In FIG. 24C, three electrodes (e.g., the first three or “proximal” electrodes) are shown as in apposition while in FIG. 24D all the electrodes are shown in apposition. In FIGS. 24E and F, the system may display certain parameters of the treatment, both during and after the treatment (e.g. power, temperature, time, and number of active/activated electrodes). Information about the treatment, such as the aforementioned parameters and/or other information, may be captured by the system and saved to memory.

Returning to FIG. 6, after the prescribed therapy in section S1 is complete, the expandable device may then be deflated and moved to an untreated section S2 to repeat the therapy applied in section S1, and similarly to section S3, and any more sections as needed. The sections are shown directly adjacent, but can be separated by some distance.

In some instances, alternative methods other than those illustrated in FIG. 6 will be utilized. For instance, in other embodiments, the treatment will be performed at only a single location in the passageway, and it will not be necessary to move the expandable device to multiple locations in the passageway.

Referring again to the example of renal hypertension involving the reduction of excessive nerve activity, the system may be used to effect a non-piercing, non-ablating way to direct energy to affect nerve activity. Accordingly the body passage shown can be a renal artery surrounded by nerve tissue N in sections S1-S3. Electrodes on the expandable device may be powered to deliver energy in the known direction of a nerve N to be affected, the depth of energy penetration being a function of energy dosage, electrode type (e.g. monopolar vs. bipolar) and electrode geometry. U.S. Pub. No. 2008/0188912 entitled “System for Inducing Desirable Temperature Effects on Body Tissue”, the full disclosure of which is incorporated herein by reference, describes some considerations for electrode geometry and the volume of tissue treatment zones that may be taken into account in some, although not necessarily all, embodiments. In some instances, empirical analysis may be used to determine the impedance characteristics of nervous tissue N such that catheter device may be used to first characterize and then treat tissue in a targeted manner as disclosed and described herein. The delivery and regulation of energy may further involve accumulated damage modeling as well.

As shown, each lesion L is created in a corresponding treatment zone A-D of the expandable device 130. Accordingly, any lesion L made in one particular treatment A-D zone will not circumferentially overlap with a lesion of an adjacent treatment zone A-D at any point along the operational axis O-O. In some embodiments, a treatment zone of the expandable device 130 can have more than one electrode pad, and thus in such cases, lesions L created by those electrode pads can circumferentially overlap. In those cases, more lesions L may be required for a particular anatomy or a pair of electrode pads are required for performing a diagnostic routine before therapy is applied. Regardless, circumferential overlap of electrodes of adjacent treatment zones will not be present.

b. Energy Delivery

Depending on the particular remodeling effect required, the control unit may energize the electrodes with about 0.25 to 5 Watts average power for 1 to 180 seconds, or with about 0.25 to 900 Joules. Higher energy treatments may be done at lower powers and longer durations, such as 0.5 Watts for 90 seconds or 0.25 Watts for 180 seconds. In monopolar embodiments, the control unit may energize the electrodes with up to 30 Watts for up to 5 minutes, depending on electrode configuration and distance between the electrodes and the common ground. A shorter distance may provide for lower energy for a shorter period of time because energy travels over more localized area with fewer conductive losses. In an example embodiment for use in renal denervation, energy is delivered for about 30 seconds at a treatment setting of about 5 Watts, such that treatment zones are heated to about 68° C. during treatment. As stated above, power requirements may depend heavily on electrode type and configuration. Generally, with wider electrode spacing, more power is required, in which case the average power could be higher than 5 Watts, and the total energy could exceed 45 Joules. Likewise, using a shorter or smaller electrode pair would require scaling the average power down, and the total energy could be less than 4 Joules. The power and duration may be, in some instances, calibrated to be less than enough to cause severe damage, and particularly less than enough to ablate diseased tissue within a blood vessel. The mechanisms of ablating atherosclerotic material within a blood vessel have been well described, including by Slager et al. in an article entitled, “Vaporization of Atherosclerotic Plaque by Spark Erosion” in J. of Amer. Cardiol. (June, 1985), on pp. 1382-6; and by Stephen M. Fry in “Thermal and Disruptive Angioplasty: a Physician's Guide”; Strategic Business Development, Inc., (1990), the full disclosure of which is incorporated herein by reference.

In some embodiments, energy treatments applied to one or both of the patient's renal arteries may be applied at higher levels than would be possible in other passageways of the body without deleterious effects. For instance, peripheral and coronary arteries of the body may be susceptible to a deleterious long-term occlusive response if subjected to heating above a certain thermal response limit. It has been discovered that renal arteries, however, can be subjected to heating above such a thermal response limit without deleterious effect.

In some embodiments, energy treatments may be applied to one or both of the patient's renal arteries to affect sympathetic nerve activity in the kidneys in order to moderate both systolic and diastolic forms of CHF. The application of therapeutic thermal energy to the tissues proximate the renal artery may be effective in reducing the sympathetic nerve activity so as to mitigate the biological processes and the resulting effects of CHF. In some embodiments, a mild application of a controlled dose of thermal energy in a rapid procedure (e.g. 10 minutes or less of therapy time per kidney) is used so as to provide a simple procedure for the clinical staff while providing a procedure that minimizes the pain felt by a patient while maximizing the efficacy of the procedure. The balloon-mounted electrodes and energy delivery methods of the present disclosure may be particularly well suited for the application of energy to reduce sympathetic nerve activity related to chronic hypertension, in conjunction with or separate from, systolic and diastolic CHF.

In some embodiments, the electrode pads described herein may be energized to assess and then selectively treat targeted tissue to achieve a desired therapeutic result by a remodeling of the treated tissue. For example, tissue signature may be used to identify tissue treatment regions with the use of impedance measurements. Impedance measurements utilizing circumferentially spaced electrodes within a body passage may be used to analyze tissue. Impedance measurements between pairs of adjacent electrodes may differ when the current path passes through diseased tissue, and when it passes through healthy tissues of a luminal wall for example. Hence, impedance measurements between the electrodes on either side of diseased tissue may indicate a lesion or other type of targeted tissue, while measurements between other pairs of adjacent electrodes may indicate healthy tissue. Other characterization, such as intravascular ultrasound, optical coherence tomography, or the like, may be used to identify regions to be treated either in conjunction with, or as an alternate to, impedance measurements. In some instances, it may be desirable to obtain baseline measurements of the tissues to be treated to help differentiate adjacent tissues, as the tissue signatures and/or signature profiles may differ from person to person. Additionally, the tissue signatures and/or signature profile curves may be normalized to facilitate identification of the relevant slopes, offsets, and the like between different tissues. Impedance measurements can be achieved at one or more frequencies, ideally two different frequencies (low and high). Low frequency measurement can be done in range of about 1-10 kHz, or about 4-5 kHz and high frequency measurement can be done in range of about 300 kHz-1 MHz, or between about 750 kHz-1 MHz. Lower frequency measurement mainly represents the resistive component of impedance and correlates closely with tissue temperature where higher frequency measurement represents the capacitive component of impedance and correlates with destruction and changes in cell composition.

Phase angle shift between the resistive and capacitive components of impedance also occurs due to peak changes between current and voltage as result of capacitive and resistive changes of impedance. The phase angle shift can also be monitored as means of assessing tissue contact and lesion formation during RF denervation.

In some embodiments, remodeling of a body lumen can be performed by gentle heating in combination with gentle or standard dilation. For example, an angioplasty balloon catheter structure having electrodes disposed thereon might apply electrical potentials to the vessel wall before, during, and/or after dilation, optionally in combination with dilation pressures which are at or significantly lower than standard, unheated angioplasty dilation pressures. Where balloon inflation pressures of 10-16 atmospheres may, for example, be appropriate for standard angioplasty dilation of a particular lesion, modified dilation treatments combined with appropriate electrical potentials (through flexible circuit electrodes on the balloon, electrodes deposited directly on the balloon structure, or the like) described herein may employ from 10-16 atmospheres or may be effected with pressures of 6 atmospheres or less, and possibly as low as 1 to 2 atmospheres. Such moderate dilation pressures may (or may not) be combined with one or more aspects of the tissue characterization, tuned energy, eccentric treatments, and other treatment aspects described herein for treatment of body lumens, the circulatory system, and diseases of the peripheral vasculature.

In many embodiments, gentle heating energy added before, during, and/or after dilation of a body lumen may increase dilation effectiveness while lowering complications. In some embodiments, such controlled heating with a balloon may exhibit a reduction in recoil, providing at least some of the benefits of a stent-like expansion without the disadvantages of an implant. Benefits of the heating may be enhanced (and/or complications inhibited) by limiting heating of the adventitial layer below a deleterious response threshold. In many cases, such heating of the intima and/or media may be provided using heating times of less than about 10 seconds, often being less than 3 (or even 2) seconds. In other cases, very low power may be used for longer durations. Efficient coupling of the energy to the target tissue by matching the driving potential of the circuit to the target tissue phase angle may enhance desirable heating efficiency, effectively maximizing the area under the electrical power curve. The matching of the phase angle need not be absolute, and while complete phase matching to a characterized target tissue may have benefits, alternative systems may pre-set appropriate potentials to substantially match typical target tissues; though the actual phase angles may not be matched precisely, heating localization within the target tissues may be significantly better than using a standard power form.

In some embodiments, monopolar (unipolar) RF energy application can be delivered between any of the electrodes on the balloon and return electrode positioned on the outside skin or on the device itself, as discussed above. Monoploar RF may be desirable in areas where deep lesions are required. For example, in a monopolar application, each electrode pair may be powered with positive polarity rather than having one positive pole and one negative pole per pair. In some embodiments, a combination of monopolar and bipolar RF energy application can be done where lesions of various depth/size can be selectively achieved by varying the polarity of the electrodes of the pair.

c. Target Temperature

The application of RF energy can be controlled so as to limit a temperature of target and/or collateral tissues, for example, limiting the heating of target tissue such that neither the target tissue nor the collateral tissue sustains irreversible thermal damage. In some embodiments, the surface temperature range is from about 50° C. to about 90° C. For gentle heating, the surface temperature may range from about 50° C. to about 70° C., while for more aggressive heating, the surface temperature may range from about 70° C. to about 90° C. Limiting heating so as to inhibit heating of collateral tissues to less than a surface temperature in a range from about 50° C. to about 70° C., such that the bulk tissue temperature remains mostly below 50° C. to 55° C., may inhibit an immune response that might otherwise lead to stenosis, thermal damage, or the like. Relatively mild surface temperatures between 50° C. and 70° C. may be sufficient to denature and break protein bonds during treatment, immediately after treatment, and/or more than one hour, more than one day, more than one week, or even more than one month after the treatment through a healing response of the tissue to the treatment so as to provide a bigger vessel lumen and improved blood flow.

In some embodiments, the target temperature may vary during the treatment, and may be, for instance, a function of treatment time. FIG. 7 illustrates one possible target temperature profile for a treatment with a duration of 30 seconds and a twelve second ramp up from nominal body temperature to a maximum target temperature of about 68° C. In the embodiment shown in FIG. 7, the target temperature profile during the twelve second ramp up phase is defined by a quadratic equation in which target temperature (T) is a function of time (t). The coefficients of the equation are set such that the ramp from nominal body temperature to 68° C. follows a path analogous to the trajectory of a projectile reaching the maximum height of its arc of travel under the influence of gravity. In other words, the ramp may be set such that there is a constant deceleration in the ramp of temperature (d²T/dt²) and a linearly decreasing slope (dT/dt) in the temperature increase as 12 seconds and 68° C. are reached. Such a profile, with its gradual decrease in slope as it approaches 68° C., may facilitate minimizing over and/or undershoot of the set target temperature for the remainder of the treatment. In some embodiments, the target temperature profile of FIG. 7 will be equally suitable for bipolar or monopolar treatments, although, in at least some monopolar embodiments, treatment time may be increased.

FIGS. 8, 9, and 10 illustrate additional target temperature profiles for use in various embodiments of the disclosure. FIG. 8 illustrates profiles with varying rise times and set target temperatures (e.g. one profile with an approximately 3 second rise time and 55° C. set temperature, one with a 5 second rise time and 60° C. set temperature, one with an 8 second rise and 65° C. set temperature, one with a 12 second rise and 70° C. set temperature, and one with a 17 second rise and 75° C. set temperature).

FIGS. 9 and 10 illustrate temperature profiles that utilize different rise profiles, some of which approach the set target temperature relatively aggressively (e.g., the “fast rise” profiles), others of which approach the set target temperature less aggressively (e.g., the “slow rise” profile). It has been experimentally determined that the “medium enhanced rise” temperature profile shown in FIG. 10 provides optimal results for at least some treatment protocols, although not all embodiments of the present disclosure are limited to this temperature profile, and different treatments and different circumstances may advantageously use other profiles. The medium enhanced rise may be an example embodiment in that it efficiently warms target tissue to the target temperature while avoiding the deleterious microscopic thermal damage that a more aggressive heating profile may cause while also providing for an optimized overall treatment time. For each of the target temperature profiles shown, a temperature ramp embodying or approximating a quadratic equation may be utilized, however, any function or other profile that efficiently heats tissue, optimizes treatment time, and avoids thermal damage to target tissue may be used. However, in still other embodiments, it will not be necessary to utilize a temperature profile that achieves all of these goals. For instance and without limitation, in at least some embodiments, optimization of treatment time may not be essential.

Both bench top and animal experimentation were undertaken to optimize and verify the target temperature profile used in denervation embodiments of the Vessix system. The following summarizes the bench top experimentation and analysis supporting the selection of the medium enhanced rise temperature profile as an example embodiment.

The tests were carried out to determine which rise time algorithm would provide optimal levels of effectiveness and safety. Some previous rise time algorithms had simply gone up to the set temperature as fast as possible, and it was believed that this was not necessarily the best course of action in at least some circumstances. Efficacy was qualitatively assessed with three dimensionless parameters. The objective was to determine the algorithm that would produce the least amount of charring, denaturing, and dehydrating of the tissue at the treatment zone, based on visual inspection, while also providing good efficacy.

A water bath was brought up to 37° C. to simulate body temperature, and a liver sample was placed in the bath to simulate conditions in vivo. Good apposition of the device was verified by noting the impedance values of the electrode-tissue interface of each bipolar electrode pair in contact with tissue. A higher impedance (>500 Ohms) was used as the benchmark for good apposition.

After the temperature profiles of FIGS. 9 and 10 were run, the liver specimen was measured at each treatment site for the length and width of the lesion at the surface, the depth of penetration, and length and width of the lesion at a 2 mm depth. The analyst had no knowledge of which treatments had been done in which order so as to reduce reporting bias. Any observations of significant tissue damage were also recorded.

FIGS. 11 and 12 show in tabular form efficacy metrics that were created to relate depth of penetration to other efficacy measures. The first is depth of penetration divided by the square root of the area of the lesion at the surface. This metric relates the depth to the lesion damage on the surface to the area of the surface lesion in a non-dimensional form. A value of 100% means that the depth of penetration was equal to the average size of the surface lesion. The next metric is area at 2 mm divided by the area at the surface. This metric reveals how well the heat is penetrating the tissue. A value of 100% means that the areas at 2 mm deep and surface area are the same. The last metric is depth of penetration times the width of the lesion at 2 mm divided by the area at the surface. This number provides information about the general shape of the lesion, and whether the energy tends to propagate radially from the electrode or pierce the tissue. A value of 100% means that the cross sectional area of lesion size was equal to the size of the surface of the lesion.

After carefully reviewing all of the experimental data, it was decided that the medium enhanced rise profile was the best temperature rise algorithm to use for certain embodiments, although, again, other target temperature profiles may also be appropriately used in conjunction with the disclosed embodiments of the present disclosure.

d. Control Algorithm

FIGS. 13 and 14 illustrate one embodiment of a method for controlling energy application of an electrosurgical device, such as those described above and shown in FIGS. 1-6, or other devices, based on a target temperature profile, such as those described above and shown in FIGS. 7-10, or other profiles. The control method may be executed using the processing functionality of the control unit 110 of FIG. 1 and/or control software, described in further detail above, or in other manners. In at least some instances, the control method provides for fine regulation of temperature or other treatment parameter(s) at the various treatment sites of the device, while utilizing a relatively simple and robust energy generator to simultaneously energize several of the electrodes or other delivery sites at a single output setting (e.g. voltage), which may minimize cost, size and complexity of the system. The control method may minimize deviation from target temperature or other treatment parameter(s), and hence minimize variation in demand on the energy generator (e.g. voltage demand) during any time slice of the treatment.

In some embodiments, it will be desirable to regulate the application of RF or other energy based on target temperature profiles such as those described above to provide for a gentle, controlled, heating that avoids application of high instantaneous power and, at a microscopic level, associated tissue searing or other damage, which could undesirably result in heat block or otherwise cause a net reduction in thermal conduction heat transfer at the device/tissue interface. In other words, by avoiding higher swings in temperature and the resultant heavier instantaneous application of energy to reestablish temperature near the target temperature, tissue integrity at the immediate interface location may be preserved. Tissue desiccation may result in a net loss of thermal conductivity, resulting in reduced effective transfer of gentle, therapeutic delivery of energy to target tissues beyond the electrode/tissue interface.

Those of skill in the art will appreciate that although the particular control method of FIGS. 13 and 14 is presented for purposes of illustration in the context of the particular electrosurgical devices already described above, that these control methods and similar methods could be beneficially applied to other electro-surgical devices.

In general, the control method embodiment of FIGS. 13 and 14 seeks to maintain the various treatment sites at a pre-defined target temperature, such as at one of the target temperature profiles of FIGS. 7-10. It does so in this embodiment primarily by regulating output voltage of the RF generator and determining which of the electrodes will by energized at a given time slice (e.g. by switching particular electrodes on or off for that cycle).

The output setting of the generator and switching of the electrodes may be determined by a feedback loop that takes into account measured temperature as well as previous desired output settings. During a particular treatment cycle (e.g. a 25 millisecond slice of the treatment), each of the electrodes may be identified for one of three states: off, energized, or measuring. In some embodiments, electrodes will only be in energized and/or measuring states (an electrode that is energized may also be measuring) if they meet certain criteria, with the default electrode state being off. Electrodes that have been identified as energized or measuring electrodes may have voltage applied or be detecting temperature signals for a portion of the cycle, or for the entire cycle.

The control loop embodiment of FIGS. 13 and 14 is designed to keep as many candidate electrodes as possible as close to target temperature as possible while minimizing variations in temperature and hence minimizing variations in voltage demand from treatment cycle to treatment cycle. FIG. 15 shows an exemplar time/temperature plot over four treatment cycles for an electrode illustrating how one embodiment of a control algorithm maintains the target temperature.

The control loop embodiment of FIGS. 13 and 14 will now be described in detail.

As indicated at step 1300, each electrode is initially set to off. At step 1302, one of the electrodes is designated as a primary electrode for that treatment cycle. As discussed in further detail below, during the treatment, the primary electrode designated will vary from treatment cycle to treatment cycle (e.g. cycle through all of the available electrodes). The determination of which electrode will be designated as the primary electrode may be done by accessing a look-up table or using any other suitable functionality for identifying a primary electrode and varying the choice of primary electrode from treatment cycle to treatment cycle.

At step 1302, additional electrodes may also be designated as candidate electrodes for energization and/or measuring during that treatment cycle. The additional electrodes designated may be candidates by virtue of being in a certain relationship or lacking a certain relationship relative to the designated primary electrode for that treatment cycle.

For instance, in some bipolar electrode embodiments, some of the electrodes on the electro-surgical device may be arranged in a manner such that there may be a potential for current leakage between the primary electrode and those other electrodes if both the primary electrode and those additional electrodes are energized simultaneously in a treatment cycle, which may undesirably cause interference with the temperature measurement by the associated heat sensing device, imprecision in the amount of energy delivered at each electrode, or other undesirable consequences. For instance, in the embodiment illustrated in FIG. 1C, if electrode pad 150 c is designated as a primary electrode, electrode pads 150 d and 170 d, which have negative poles immediately adjacent or proximate the positive pole of electrode pad 150 c, may be considered to be not candidates for measuring and/or energization for that particular treatment cycle, since they are leakage-inducingly proximate to the designated primary electrode. Additionally, in this embodiment, electrode pad 150 b, which has a positive pole immediately adjacent or proximate the negative pole of electrode pad 150 c, may be considered to not be a candidate, since it is also leakage-inducingly proximate to the designated primary electrode. Furthermore, in this particular embodiment, electrode pad 170 b would also be considered a non-candidate because it is on the same flex structure as the leakage-inducingly proximate electrode pad 150 b. Finally, in this particular embodiment, electrode pads 150 a and 170 a would be considered candidates because they are adjacent non-candidates.

As another non-limiting example, in some monopolar electrode embodiments, the candidate electrodes are the monopolar electrodes that have similar measured or estimated electrical circuit properties to one or more measured or estimated properties of the electrical circuit associated with the primary electrode. In other words, in some monopolar systems, it may be desirable to only simultaneously energize monopolar electrodes that define substantially similar electrical circuits to the electrical circuit defined by the primary monopolar electrode (e.g. the circuit defined by the monopolar electrode, the common electrode, and a pathway through the patient's tissue). In some instances, this may facilitate uniformity in current flow during energization. In other embodiments, a pre-defined table or other listing or association will determine which electrodes are candidate electrodes based on the current primary electrode.

In at least some embodiments, switches associated with non-candidates will be opened to isolate the non-candidates from the rest of the system's circuitry. This switching, in at least some embodiments, could also or alternatively be used to otherwise maximize the number of available electrode pairs available for energization provided that a common ground between pairs is not affected by the switching off.

In other embodiments, the electro-surgical device may be configured to avoid the potential for leakage or otherwise take such leakage into account, and, accordingly, all the electrodes of the device may be candidates for energization and/or measuring during a treatment cycle.

In some embodiments, the assignment of an electrode as either the primary electrode, candidate, or non-candidate may be determined by a sequence matrix or look up table in an array that identifies the status of each of the electrodes and an order for the designation of primary electrodes. In one non-limiting embodiment, the primary electrode designation cycles circumferentially through the proximate electrodes and then circumferentially through the distal electrodes (e.g. in FIG. 1C, the sequence may be 170 a, b, c, d, 150 a, b, c, d). However, any pattern or other methodology could be used including ones that optimize distance between the next in sequence, the nearness of next in sequence, or the evenness of distribution.

In some embodiments, additional conditions may result in a particular electrode being set to off for a particular treatment cycle and/or for the remainder of the treatment. For instance, as discussed below, during the course of treatment, as much as 4° C. temperature overshoot may be allowed (e.g., even if such overshoot results in the electrode not being energized, it will not necessarily be set to off and still available for measuring); however, in at least some embodiments, if eight consecutive treatment cycles measure temperature overshoot for a particular electrode, that electrode will be set to off for the remainder of the treatment, with the treatment otherwise continuing and without otherwise changing the control loop process discussed below.

At step 1304, target voltages for each of the primary and other candidate electrodes are determined. In this particular embodiment, a target voltage for a particular electrode may be determined based on a temperature error associated with the treatment site of that electrode as well as the last target voltage calculated (although not necessarily applied) for that electrode. Temperature error may be calculated by measuring the current temperature at the treatment site (e.g. utilizing the heat sensing device associated with the electrode proximate that treatment site) and determining the difference between the measured temperature and the target temperature for that instant of time in the treatment.

Those of skill in the art will appreciate that while this particular embodiment is described as using voltage as a control variable, that power could be used as an alternative to voltage for the control variable, based on, for instance, a known relationship between power and voltage (i.e. power equaling voltage times current or impedance).

FIG. 14 illustrates one embodiment of a sub-routine for determining a target voltage for an electrode. At 1402, a temperature error from target (T_(e)) is calculated by subtracting the target temperature at that time (T_(g)) from the actual temperature (T) (e.g. as measured by a thermistor associated with that electrode). At 1404, it is determined whether the temperature error calculated at 1402 is greater than 4° C. (i.e. if the target temperature is 68° C., determining if the temperature as measured by the thermistor is above 72° C.). If the temperature error is greater than 4° C., the sub-routine assigns that electrode a target voltage of zero for that treatment cycle at 1406. If the temperature error is not greater than 4° C., the subroutine proceeds to 1408 and determines whether the temperature error is greater than 2° C. If the temperature error is greater than 2° C., at 1410, the sub-routine assigns that electrode a target voltage of 75% (or another percentage) of the last assigned target voltage for that electrode. If the temperature error is not greater than 2° C., at 1412, the sub-routine may assign a target voltage for that electrode based on the equation:

V=K _(L) V _(L) +K _(p) T _(e) +K _(I)∫^(t) _(t-n sec) T _(e AVE)

-   -   where:         -   V is the target voltage;         -   T_(e) is a temperature error from target;         -   V_(L) is the last assigned electrode voltage;         -   K_(L), K_(P), and K_(I) are constants; and         -   n is a time value ranging from 0 to t seconds.

In some embodiments, including the embodiment of FIG. 14, the equation used may be:

V = 0.75 V_(L) + K_(p)T_(e) + K_(I)∫_(t − 1 sec )^(t)T_(e AVE)

-   -   where:         -   V is the target voltage;         -   T_(e) is the temperature error from target;         -   V_(L) is the last assigned electrode voltage;         -   K_(P) is a constant from proportionate control; and         -   K_(I) is a constant from integral control.

In some embodiments, it may be beneficial to use only the last assigned electrode voltage for determining a target voltage, rather than utilizing averages of voltages or voltages from earlier treatment cycles, as, in some cases, use of earlier voltages may be a source for computational error in embodiments that focus on fine control of the target temperature.

Returning to FIG. 13, once target voltages are determined for the primary electrode and other candidate electrodes, at step 1306, it is determined whether the target voltage for the primary electrode is greater than zero. If not, at 1308, the output voltage of the RF generator is set for that treatment cycle to the lowest target voltage determined at 1304 for the other candidate electrodes. If the target voltage determined at 1304 for the primary electrode is greater than zero, at 1310, the output voltage of the RF generator is set for that treatment cycle to the target voltage of the primary electrode.

At step 1312, the primary and other candidate electrodes with a target voltage greater than zero are identified as electrodes to be energized. In alternative embodiments, candidate electrodes other than the primary will only be energized if the target voltages determined for those electrodes is 6V greater than the set voltage.

In still other embodiments, candidate electrodes other than the primary will only be energized if the target voltages determined for these electrodes are 1, 5 or 10V greater than the set voltage.

At step 1314, it is determined whether the electrodes to be energized are currently at temperatures greater than 68° C. Those electrodes that are at temperatures greater than 68° C. are switched off or otherwise prevented from being energized in that treatment cycle, and those electrodes otherwise meeting the above criteria are energized at the set voltage at step 1316. Subsequently, another treatment cycle begins, and the control loop of FIG. 13 is repeated until the treatment is complete. In some embodiments, each treatment cycle will be non-overlapping with the previous and next cycles (e.g. the steps of FIG. 13 will be completely performed before the next cycle's steps begin), although, in other embodiments, the cycles may be overlapping at least to some extent.

FIGS. 16-23 are charts of temperature (target and actual) and target voltage over time for a treatment employing a Vessix System for renal denervation that utilizes the control loop of FIG. 13 to regulate actual temperature at the device's eight electrodes to the target temperature profile. It should be understood that the target voltage charted in these Figures is not the same as the actual voltage applied to the electrodes, since, as described above, the target voltage for only one of the electrodes is used to set the actual voltage applied in each treatment cycle. As shown in FIGS. 16-23, the control loop of FIG. 13 functions to precisely maintain the actual temperature at each electrode of the device at the target temperature. As also shown in FIGS. 16-23, measured impedance may decrease in some instances over the course of the treatment (particularly at the beginning of the treatment), reflecting increased mobility of the ions in the tissue in response to the high frequency RF energy.

It has been experimentally determined that an example embodiment of the temperature control method described above, when employed as part of the Vessix System for Renal Denervation, provides effective reduction of norepinephrine (NEPI) concentration. In one experiment, efficacy and safety of the Vessix System for Renal Denervation was assessed in healthy juvenile Yorkshire swine at 7 and 28 days post-treatment, including an assessment of kidney NEPI concentration levels at 7 days post-treatment. FIG. 25 is a table summarizing the study design for this particular experiment. Efficacy of groups 1 and 2 was measured as percent reduction of NEPI level in the treated arteries vs. untreated contralateral control kidney in each animal at 7 days. FIG. 26 shows percent NEPI reduction of both groups (as means+/−SD). There were no significant changes in body weight, body condition score or clinical pathology parameters in any animal over the course of the study. Overall, the average baseline vessel diameters were similar amongst groups across all time points. Luminal gain or loss was calculated (average pre-necropsy−average baseline diameter) and exhibited similar luminal gains for treated vessels when compared to vessels of the animals that were not treated. Representative angiography images of the renal artery pre-treatment, 7 and 28 days post RF treatment are shown in FIGS. 27-30. No perforation, dissection, thrombus nor emboli were detected acutely or chronically via angiography analysis.

e. Nerve Signal Stimulation and Monitoring

In at least some of the embodiments described above, or in alternative embodiments, renal-denervation treatment methods and systems may provide for stimulation of nerve signals and monitoring for nerve signal response in the tissue proximate the treated renal artery. In some instances, this electrogram of neural activity may provide an assessment of the denervation treatment's efficacy and/or provide feedback for regulating the treatment. In at least some embodiments, such an electrogram provides for an assessment of whether neural activity is present and/or has shifted (e.g. decreased) relative to a measured baseline, and does not involve mapping or quantifying the presence of neural tissue proximate the renal artery.

In one embodiment, the same electrode assemblies used to deliver the denervation treatment, such as the bi-polar electrode pairs on the distal and proximal electrode pads 150 a-d and 170 a-d shown in FIG. 1C, may also be configured for stimulation of nerve signals and monitoring for nerve signal responses. For instance, one of the proximal bipolar electrode pairs on one of proximal electrode pads 150 a-d may be used to stimulate a nerve signal and one of the distal bipolar electrode pairs on one of distal electrode pads 170 a-d may be used to monitor for a nerve signal response. Alternatively, a distal bipolar electrode may be used for stimulation and a proximal bipolar electrode may be used for monitoring. In these or other embodiments, stimulation and sensing may be performed by axially or circumferentially adjacent electrode pairs.

Electrodes 222 having the size, spacing, other geometries and other characteristics as described above in the context of FIG. 2A may be sufficient for stimulation and monitoring of nerve signals, although, in alternative embodiments, the electrodes may be further reduced in size and/or other characteristics may modified to provide higher signal resolution. Other modifications to the systems and devices described herein may also be made to minimize interference with the stimulation and (particularly) monitoring of nerve signals. For instance, in some embodiments, the layout of the system's circuitry (such as the RF generator's internal circuitry) and/or the pairing, twisting, and other characteristics of the wiring associated with the catheter/flex circuitry may be optimized to reduce the inherent capacitance of the circuitry to provide for reduced electromagnetic flux.

In alternative embodiments, the electrodes used to stimulate and/or monitor for nerve signals may be different from the electrodes used to deliver the energy treatment. The stimulation/monitoring electrodes may have positions, geometries, and other characteristics optimized for stimulation/monitoring and the energy delivery electrodes may have positions, geometries and other characteristics optimized for delivering the energy treatment. FIG. 42 shows an example of a catheter including electrodes for delivering an energy treatment (similar to the electrodes shown in FIG. 10) and separate electrodes (in the form, here, of circumferential ring electrodes on distal and proximal ends of the expandable device) for stimulating and monitoring for nerve signals. FIG. 43 shows an example of a catheter including separate proximal and distal expandable devices carrying ring electrodes for stimulating and monitoring for nerve signals. The electrodes of FIGS. 42 and 43 may each be a bipolar electrode, a monopolar electrode, or may constitute a bipolar electrode between the proximal and distal electrode rings. As shown in FIG. 24D the schematic representation of electrodes may be shown on a user interface to identify electrode regions that are available to be energized, and may further include indication of sufficient tissue apposition by the measurement of impedance. Because a user interface may show electrode configurations in a schematic form, it should be understood that the schematic image should not be limiting to the types of electrode configurations present on the expandable structure. Electrodes may be any one or more of rings, bipolar pairs, point electrodes, axially elongate electrodes, and the like.

In monopolar embodiments, the electrodes serve as the positive pole for stimulating and sensing during treatment, while a separate negative pole is used as a ground. The negative pole may be located on the expandable structure, at one or more points on the catheter body, or external to the patient in the form of a grounding pad. In monopolar configurations, signal processing and filtering (as further described below) are desirable options because of the relatively large difference in magnitudes between energy delivery and nerve response detection.

The RF generator and other circuitry of the control unit 110 shown and described for FIG. 1A may be used to generate the nerve stimulation signal and monitor for the response, although, in other embodiments, a separate device may be associated with the system for generating nerve stimulation and/or monitoring response.

In one embodiment, the nerve stimulation may be a voltage in the range of about 0.1V to about 5V, or about 0.5V, applied by the first electrode for a period of about 1 second or less, or about 0.5 milliseconds, followed by a pulse width modulation, which may shock a nerve tissue into propagating a nerve signal. The pulse signal may be of any form with a square wave being one example form because the rapid on/off nature of the wave form efficiently stimulates a nerve response with no ramp to or from peak voltage.

Neural activity may be assessed by measuring one or more of amplitude of the nerve signal in response to the stimulation, speed of the nerve signal in response to the stimulation, and/or fractionated amplitude of the nerve signal. Here, a fractionated amplitude refers to a net reduction and change to the nerve conduction signal as compared to a pre-treatment baseline. A pre-treatment signal would be expected to have a relatively larger amplitude and smoother transition of slope while a signal from a nerve having received at least some treatment would be expected to have a relatively lower amplitude and a less smooth, sudden, or broken transition in slope indicative of interrupted nerve conduction due to treatment. These measurements can be determined by measuring a change in voltage at the second electrode and/or a measured time between the stimulation and the response, and, in at least some embodiments, may utilize high and/or low pass filtering to differentiate the nerve signal from background noise.

Currently, interventional energy delivery therapies such as renal denervation are performed based on anatomical landmarks. In the example of renal denervation, it is known that a majority of nerves are located along the length of renal arteries. Post treatment assessment is based on secondary effects such as NEPI and blood pressure reductions, which are not typically immediate indicators and are not indicative of nerve viability.

In the current state of the art there is no means available to directly assess functional behavior of renal nerves in real-time during a renal denervation procedure. A solution to this problem is the use of alternating current or direct current to deliver sub-threshold or low stimulation signals in the vicinity of renal nerves within renal arteries to access their activity pre and post renal denervation treatment.

High resolution rapid nerve viability measurements may be accomplished via multiple localized electrodes such as those shown in FIGS. 1B and 1C, however, it should be noted that embodiments are not limited to bipolar flex circuit electrodes on balloons. Any electrode configuration (monopolar or bipolar) suitable to be mounted to a catheter-based expandable structure may be employed; ring electrodes, linear or spiral electrodes, point electrodes, and the like, may be mounted to baskets, balloons, or any other such type of structure used in catheter systems.

The measurement technique employs electric stimulation from at least one electrode over the path of a nerve to evoke the generation of an action potential that spreads along the excited nerve fibers. That action potential is then recorded on another point. This technique may be used to determine the adequacy of the conduction of the nerve impulse as it courses down a nerve, thereby detecting signs of nerve injury. The distance between electrodes and the time it takes for electrical impulses to travel between electrodes are used to calculate the speed of impulse transmission (nerve conduction velocity). A decreased speed of transmission indicates nerve damage.

Velocity, amplitude, as well as shape of the response following electrical stimulation of renal nerves will be measured via multiple electrodes on the balloon catheter. Abnormal findings include conduction slowing, conduction blockage, lack of responses, and/or low amplitude responses

Referring to FIGS. 44 and 45, electrical signal morphology is indicative of a change in nerve conduction as evidenced by the change in the degree of fractionation combined with slow conduction. FIG. 44 shows a representative nerve signal 4401 in the pre-treatment or baseline condition. FIG. 45 shows a representative nerve signal 4501 after having received at least some energy treatment. When comparing signal 4401 to signal 4501, it is evident that the amplitude of the nerve signal has been reduced while the pulse width has been increased. It is also evident that the slopes and changes in slopes of the signal 4501 are much less smooth than the slopes and changes in slopes of the signal 4401. This is illustrative of how a nerve responds to the energy treatment of the subject disclosure; as energy is delivered the nerve conductive properties are reduced or eliminated thereby causing the nerve signals to be reduced, less continuous, and slower in velocity.

Nerve signal measurement may be optimized using signal filtering such that the influence of cardiac electrical signals, stimulation signals, and system noise are filtered out of the nerve sensing circuit so as to optimize the accuracy and sensitivity of the circuit. Signal filtering may be accomplished through means such as band-pass filters. For example, a low-pass filter in the range of about 1 Hz to about 500 Hz, with an example value of 100 Hz and a high-pass filter in the range of about 1 kHz to about 10 kHz, with an example value of 5 kHz may be employed to establish the frequency band of signals to be sensed and measured by the circuit. Measurements are then used as feedback applied to the energy control algorithm used to regulate the delivery of therapeutic energy.

In a monopolar embodiment sensing is from a broader field of tissue because energy flows from the one or more positive poles of electrodes to the negative pole or poles of a common grounding path. Applying this concept to the embodiment of FIGS. 1B and 1C, an example polarity would be to use an external patch (not shown) as the positive pole while the electrode assemblies 140 a-d serve as the negative poles of a common grounding circuit used for nerve signal measurement. In this seemingly backward application of energy for the purposes of sensing, the electrode assemblies 140 a-d are more proximate to the nerve tissue of interest and hence may provide improved sensing accuracy by serving as negative poles for sensing. During the energy delivery mode of treatment, the polarities of the external patch and electrode assemblies 140 a-d may be switched such that the electrode assemblies 140 a-d are the positive poles and the external patch is the negative pole for grounding.

In a bipolar embodiment, sensing is from a localized field of tissue because the positive and negative poles of electrode assemblies 140 a-d are immediately adjacent, and hence, the tissue volume sensed is much more localized than in a monopolar configuration. The close proximity of electrode poles in a bipolar arrangement may be desirable because the proximity of poles allows for an inherently lower quantity of energy delivery to energize tissue and an inherently higher degree of measurement resolution because of the smaller tissue volume between poles. Additionally, the electrode assembly 140 a-d configurations provide a proximal/distal linear spacing that allows for the sensing and measuring the linear travel of a nerve signal along a path as has been described herein.

Nerve signal stimulation and measurement may occur before, during, and/or after the energy treatment. In one embodiment, neural activity is assessed prior to treatment to establish a baseline level of neural activity and is then reassessed after the treatment to determine whether a threshold level of change in neural activity has resulted. Any one or more of percentage reduction in nerve signal amplitude, degree of fractionation of signal slope, increase in duration of nerve signal pulse, and increase in time between nerve signal pulses may be used to measure a tissue response indicating that denervation in the target tissue has occurred or is in the process of occurring. In other words, total disruption of nerve activity may be a delayed response to the denervation treatment, although some decrease in nerve activity may occur during or just after the denervation treatment sufficient to indicate the effectiveness of the treatment. In alternative embodiments, an effective denervation may be characterized as one in which no nerve signal is detected in response to a pre-determined stimulation.

Nerve signal assessment may also or alternatively be conducted during the energy treatment. For instance, the control algorithm shown in FIG. 13 may be modified to allow time scale measurements of stimulated nerve activity (such measurements being on the order of any of milliseconds, microseconds, nanoseconds, picoseconds, etc.) prior to or after each electrode firing cycle. These intra-cycle measurements may be compared to a pre-treatment baseline, to measurements from earlier cycles, or to other standards.

In some embodiments, regardless of whether the nerve activity assessment is conducted pre and post treatment, periodically between each treatment cycle, or periodically after a certain number of treatment cycles, data from the neural activity assessments may be used to establish or adjust parameters for the denervation treatment. For instance, in the embodiment illustrated by FIGS. 13 and 14, while the set voltage for each cycle may be a function of previous voltage applied and measured and averaged temperature errors, total time at the treatment temperature may be a function of measured neural activity, or a function of deviation of measured neural activity from an earlier measured or pre-set baseline. One or more of measured amplitude of the nerve signal, speed of the nerve signal, and/or fractionated amplitude may be accounted for in such an algorithm. Thus, if a significant decrease in neural activity is measured early in the denervation treatment, the total treatment time may be shortened. Conversely, if the nerve signal assessments are not measuring a decrease in neural activity, the total treatment time may be lengthened. Of course, feedback from the nerve signal assessment(s) may be used to vary additional or alternative parameters of the denervation treatment.

Measuring of nerve signals may be directly integrated into the energy delivery and control methods described herein. As candidate electrodes are selected and energized in accordance with the control algorithm, the additional function of nerve signal measuring may be integrated into the control algorithm such that the additional control factor of nerve response increases the precision with which energy is delivered and a therapeutic response is achieved while avoiding the delivery of excess energy in order to preserve pre-treatment issue cellular state to the maximum degree possible. As shown in FIG. 13A, an additional control loop step 1313 may be used to evaluate whether the nerve signal reduction threshold has been met. If the nerve signal reduction threshold is not met, the control loop then advances to loop step 1314 to determine whether a candidate electrode has reached a temperature threshold. If at loop step 1313 a nerve is determined to have reached the signal reduction threshold, then the electrode may be deselected as a candidate electrode to be energized.

Treatment of Small/Branched Vessels and Other Passageways

The systems and devices described herein may be advantageously used in situations where other energy-based treatment systems and devices would not be suitable. For instance, embodiments of the systems and devices described herein may be used in vessels and other passageways that are too small for treatment using other catheter-based energy treatment systems. In some instances, the systems and devices described herein may be used in renal arteries or other vessels having diameters of less than 4 mm and/or lengths of less than 20 mm. Other factors, such as vessel tortuosity and proximity of the treatment site to regions that should not receive treatment, may be contra-indications for or otherwise not suitable for treatment using earlier devices but not for at least some embodiments of the presently described systems and devices.

FIGS. 1D and E show 4 and 5 mm balloons with three electrode assemblies each. The particular geometries of these electrode assemblies and other characteristics described in preceding sections, however, facilitate their use on smaller diameter balloons, such as 1, 2 or 3 mm balloons or intermediate sizes thereof. In some instances (such as in some 1 mm embodiments), the balloon may not include a guidewire lumen. FIG. 46 shows one embodiment of a balloon with the main body 4601 being made of Kapton® a flexible polyimide film available from DuPont™, with the shoulders 4602 being made of a standard balloon material. In some instances, the Kapton® body of the balloon of FIG. 46 may be used to eliminate the need for a separate layer of the flexible circuit assemblies used on the balloon, such as to eliminate the base layer 202 shown in FIG. 2B, thereby reducing the profile of the flexible circuit assembly.

Other features of the systems and devices described above may also facilitate their use in vessels that are relatively small. For instance, delivering an energy treatment to a small diameter vessel may require particularly fine control over the amount of energy delivered and/or the temperature increase caused by the treatment. As such, the particular electrode energy delivery geometries, control algorithms, and other features described above may make the present systems and devices particularly suitable in such situations.

FIG. 47 schematically shows a typical primary renal artery 4701 branching from the aorta 4702 to the kidney 4703. An embodiment of the present disclosure is shown where the balloon and electrode assembly 4704 of the catheter is expanded and positioned for treatment of tissue. An energy dose is applied and the balloon is subsequently deflated and removed or repositioned.

FIG. 48 schematically shows a primary 4801 and an accessory renal artery 4802 branching from the aorta 4803 with both extending to the kidney 4804. Accessory arteries may range in size from about 1 mm in diameter to about 5 mm in diameter. The renal arteries of FIG. 48 should be understood to be a simple schematic representation of what may vary from subject-to-subject in vivo. For instance, the arteries may vary in diameter, length, tortuosity, location, and number. Furthermore, these variations may be with respect to each artery as well as with respect to each subject. FIG. 48 shows a first balloon catheter A positioned for treatment in a smaller accessory artery and a second balloon catheter B positioned for treatment in a larger primary renal artery.

In practice, it may be possible that catheter A and catheter B are one in the same if the two arteries are sufficiently close in diameter to allow for complete balloon expansion and contact with the tissue of the arterial lumens. It may be further possible that catheter A and catheter B may be repositioned along the length of the respective arteries depending on the treatable length of each artery. It may also be further possible that the primary and accessory arteries may be treated simultaneously should a physician so desire.

To applicant's knowledge, prior to the present disclosure, the treatment of accessory renal arteries has not been possible because of technological limitations caused by overheating of small arteries, space constraints when operating in luminal areas with smaller cross sections, and the difficulty of navigating tortuous pathways. Because the embodiments of the present disclosure use expandable, catheter-based structures, flexible circuit electrodes on balloons, the limitations of “one size fits all” devices are obviated. Balloon and electrode assemblies of the present disclosure are incrementally sized and arranged to facilitate the precisely controlled thermal energy dose for an incremental range of luminal diameters. In other words, the balloon and electrode assembly is incrementally sized and arranged for optimized operation in a correspondingly sized lumen. The number of electrodes is chosen to avoid overheating of tissues. The balloon-based expandable structure is able to navigate to a location at a smaller, unexpanded diameter with flexibility. The large surface contact of an expanded balloon allows for uniformity in tissue contact while avoiding the bending and/or tight space constraints of single point probes or other such similar designs.

Accessory renal arteries are present in 25-30% of human patients; however these patients have been excluded from previous renal denervation studies. Within the REDUCE-HTN Clinical Study (the full contents of Vessix Vascular clinical study protocol CR012-020 being incorporated herein by reference) a subset of four subjects underwent successful treatment of primary and, at least, one accessory renal artery using the Vessix Renal Denervation System (Vessix Vascular, Inc.; Laguna Hills, Calif.) that includes a 0.014 inch over-the-wire percutaneous balloon catheter with up to 8 radiopaque gold electrodes mounted on the balloon surface in a longitudinally and circumferentially offset pattern. In an exemplary embodiment, a catheter is connected to a proprietary automated low-power RF bipolar generator that delivers a temperature-controlled therapeutic dose of RF energy at about 68° C. for about 30 seconds. The mean baseline office-based blood pressure (OBP) of this cohort was 189/93 mmHg. In addition to an average of 10.5 denervations of each main renal artery, this cohort was treated with an average of 8 denervations per accessory renal artery.

In this study, for the four subjects, no peri-procedural complications were reported and immediate post-procedure angiography indicated no renal artery spasm or any other deleterious effects. These four subjects demonstrated improvement at two weeks post-procedure with a mean reduction in OBP of −32/−16 mmHg (190/97 to 167/91; 175/92 to 129/70; 192/94 to 179/91; 183/87 to 138/55).

FIGS. 49 and 50 schematically illustrate non-limiting examples of renal denervation treatments where energy delivery is selectively delivered using a subset of the electrodes of an electrode assembly. FIG. 49 schematically illustrates a renal artery 4901 that includes a branch 4902. In this instance, the balloon and electrode assembly 4903 is positioned in the renal artery such that one of the electrodes 4904 is proximate an ostium joining the branch to the renal artery, and thus is not in apposition with a vessel wall. As described above in some embodiments, systems and methods in accordance with the present disclosure may be configured to selectively energize the electrodes or a subset of electrodes in apposition with the vessel wall (e.g. electrodes 4905 and 4906 in FIG. 49) while not energizing the electrodes or a subset of electrodes that are not in apposition with a vessel wall (e.g. electrode 4904). Those of skill in the art will appreciate that, in addition to the example of FIG. 49, a variety of other factors could result in less than complete apposition between the electrode assembly and vessel wall, including, without limitation, vessel tortuosity, changes in vessel diameter, presence or absence of buildup on the vessel wall, etc.

FIGS. 50A and B schematically illustrate a non-limiting example of a renal denervation treatment where an energy treatment is performed with the electrode assembly and balloon at two positions in a renal artery 5001. In FIG. 50A, the balloon is positioned such that all of the electrodes 5002-5005 are in the renal artery 5001 and are potential candidates for energization. In FIG. 50B, after an energy treatment has been performed at the position shown in FIG. 50A, the balloon and electrode assembly has been withdrawn such that a portion of it remains in the renal artery 5001 and a portion of it is in the aorta 5006. In the positioning shown in FIG. 50B, certain embodiments of systems and methods of the present disclosure will be configured to select only electrodes 5002 and 5005 (and any other electrodes positioned within renal artery 5001 and/or in apposition with a wall of the renal artery 5001) as potential candidates for energization, with electrodes in the aorta 5006 identified as non-candidates for energization. As illustrated by FIGS. 50A and B, certain embodiments of the present disclosure may facilitate delivering energy to tissues at or proximate the ostium joining the aorta 5006 to the renal artery 5001, which may, in at least some patients, be an area of relatively high concentration of nerve tissues.

Impedance Compensation

As indicated herein, bipolar pairs of electrodes may be used to ablate, modulate, or otherwise remodel tissue including renal nerves. At least some of the electrodes contemplated may be arranged on a flexible circuit and/or dyad 5040 schematically illustrated in FIG. 51 that can be mounted on a balloon with a distal pair of bipolar electrodes (e.g., with the pair of bipolar electrodes including one or more active electrodes and one or more ground electrodes) on a distal electrode pad 5050 and a proximal pair of bipolar electrodes (e.g., also with the pair of bipolar electrodes including one or more active electrodes and one or more ground electrodes) on a proximal electrode pad 5070. As indicated above, distal electrode pad 5050, the proximal electrode pad 5070, or both may include a temperature sensor (e.g., a thermistor).

Each dyad 5050 may utilize a common ground trace disposed on the intermediate tail 5060 that is connected to the ground electrodes disposed on distal electrode pad 5050 and to the ground electrodes disposed on proximal electrode pad 5070. The common ground may facilitate current leakage from electrode pad 5050 to electrode pad 5070, particularly when electrode pad 5050 is activated. In one example, current may pass from the active electrode(s) of distal electrode pad 5050 to the ground electrode of proximal electrode pad 5070 when the distal pair of bipolar electrodes is fired or otherwise activated. If this occurs, the impedance measured at the distal electrode pad may not be as accurate because of this current leakage. If the accuracy of the measured impedance is off significantly due to current leakage to an adjacent electrode pad, the system may classify a given electrode pad as not being in contact with the renal artery, only partially in contact with the renal artery, or disposed within the aorta in the blood stream away from the renal artery. In some instances, this could lead to the system incorrectly identifying the electrode pad as not being suitable for activation due to not being in contact with the wall of the renal artery. Accordingly, the system may not perform therapy at the electrode when therapy may have been appropriate. Alternatively, the system may perform therapy at the electrode when therapy may not have been appropriate.

In order to compensate for the possibility of current leakage, a control unit may be configured to take into account the possibility of current leakage by “compensating” the impedance measurements. An illustrative control unit 110 is shown in FIG. 53. The illustrative control unit 110 may include an input/output block 5400 for electrically connecting the control unit 110 to an in vivo medical device, such as catheter device 120. The control unit may also include a controller 5402 that is communicatively coupled to the input/output block 5400. A memory 5404 may be coupled to the controller 5402 as shown. The memory 5404 may store program code, data (such as look-up tables or the like) and/or any other temporary or permanent information. The particular compensation process may depend on the particular medical device 110. In one example, the control unit 110 may be used with a variety of different catheter devices 120, such as catheter devices having different sizes and/or numbers of dyads.

In some instances, the process may include taking an impedance measurement at a selected electrode pad of catheter device 120 (e.g., the designated electrode, which in this example may be distal electrode pad 5050), and if the impedance measurement falls within a pre-selected range of values, it may be deemed that compensation is not necessary. The range of measured impedance where compensation may be appropriate may be about 300-1000 ohms, about 400-900 ohms, about 500-850 ohms, or in any other suitable range. An impedance falling below the selected range (e.g., below 500 ohms) may be deemed to correspond to a case where the electrode pad is “not in contact” with the wall of the renal artery. Likewise, an impedance measurement falling above the selected range (e.g., above 850 ohms) may be deemed to correspond to a case where the electrode pad is in sufficient contact with the renal artery. For reference, the impedance of blood is approximately 570 ohms. If the measured impedance falls between the selected range, the control unit may calculate an impedance compensation value and adjust the measured impedance of an electrode pad accordingly. In some instances, a comparison to such an impedance range is not performed, and compensation is applied regardless.

In order to more clearly understand the impedance compensation calculation, a first model may be considered that includes dyad 5040 with a first pair of bipolar electrodes at distal electrode pad 5050 and a second pair of bipolar electrodes at proximal electrode pad 5070. The desired impedance to be measured may be the impedance between the bipolar electrodes on distal electrode pad 5050. This impedance may be designated Z₁. Leakage may occur between the active electrode(s) of bipolar electrodes of distal electrode pad 5050 and the common ground electrode(s) of the bipolar electrodes of proximal electrode pad 5070. This leakage impedance may be designated Z₁₂. The impedance measured by the control unit at the distal electrode pad 5050 may be designated measured impedance MZ₁. It can be appreciated that the measured impedance MZ₁ may represent the combination of impedance Z₁ and Z₁₂. Because these impedances Z₁ and Z₁₂ may be run in parallel, the measured impedance MZ₁ may be represented by the following equation:

(1/MZ ₁)=(1/Z ₁)+(1/Z ₁₂)  Equation (1)

Through experimentation, it has been determined that the impedance Z₁₂ may be related to (i.e. proportional to) the measured impedance MZ₂ measured at proximal electrode pad 5070 according to the following equation:

Z ₁₂ =kMZ ₂  Equation (2)

wherein k is a constant.

This relationship can be substituted into equation (1) and solved for Z₁ as follows

Z ₁=(MZ ₁)(kMZ ₂)/(kMZ ₂ −MZ ₁)  Equation (3)

where:

-   -   MZ₁ is the measured impedance between the bipolar electrodes on         distal electrode pad 5050; and     -   MZ₂ is the measured impedance between the bipolar electrodes on         proximal electrode pad 5070.

As can be seen, the measured impedance MZ₁ may be compensated using this linear equation (3) to give a better approximation of the actual impedance Z₁ between the bipolar electrodes on distal electrode pad 5050. While a linear function is shown here, it is contemplated that a non-linear function may be used. In some instance, the linear and/or non-linear function may also be a function of temperature, voltage signals applied to obtain the impedance measurements MZ₁ and/or MZ₂, and/or any other suitable parameter as desired.

Equation (3) can be solved after the value of k is known. It can be appreciated that the value of k may vary depending on a number of factors including, for example, the size of the balloon, the number of electrodes/dyad, and the like. In one example medical device, which utilizes a balloon having an outer diameter of 4 or 5 mm, the value of k may be in the range of about 2.0-4.0, or about 2.5-3.5, or about 3.0.

In some instances, the value of the constant k may depend on the measured impedance value MZ₁ and/or MZ₂. For example, the constant k may be a function of the measured impedance value MZ₂ as follows:

k=f(MZ ₂)  Equation (4)

In another example, the constant k may be a function of the measured impedance value MZ₁ and MZ₂ as follows:

k=f(MZ ₁ ,MZ ₂)  Equation (5)

In this example, the control unit may include a memory that stores a look-up table, wherein the measured impedance values MZ₁ and/or MZ₂ may be used to index into the look-up table to find an appropriate value for the constant k.

In some cases, two different constants k₁ and k₂ may be used. In this example, the impedance Z₁ may be expressed as:

Z ₁=(k ₁ MZ ₁)(k ₂ MZ ₂)/(k ₂ MZ ₂ −k ₁ MZ ₁)  Equation (6)

In the above examples, the control unit may be utilized to perform these calculations and adjust or compensate the measured impedance MZ₁ as necessary in order to more accurately determine the impedance Z1 of the corresponding electrode pad, and thus whether or not the given electrode pad is suitably in contact with a surface such as a renal artery so as to allow an effective therapy.

It can be appreciated that an analogous compensation calculation can be utilized when proximal electrode pad 5070 is fired (e.g., where the measured impedance is represented by the impedance Z₂ between the bipolar electrode pairs on proximal electrode pad 5070 and the impedance Z₂₁ between the active electrode on proximal electrode pad 5070 and the ground electrode on distal electrode pad 5050.

In one example, as the size of the balloon and/or the number of dyads is altered, the calculation may be adapted accordingly, such as to account for more than one potential leakage pathway when compensating the measured impedance of a corresponding electrode pad. For example, in an example medical device including a 6-7 mm outer diameter balloon with a total of four dyads (8 total pairs of bipolar electrodes), leakage can occur not only between pairs of electrodes on the same dyad but also with the bipolar pairs of electrodes on the dyad on the opposite side of the balloon, particularly wherein these dyads share a common ground.

FIG. 52 schematically illustrates four example dyads 5140 a/5140 b/5140 c/5140 d that may be disposed on the outer surface of a balloon. In this example, dyads 5140 a and 5140 c are on opposite sides of the balloon. Similarly, dyads 5140 b and 5140 d are on opposite sides of the balloon. Each of the dyads 5140 a/5140 b/5140 c/5140 d may include a distal electrode pad 5150 a/5150 b/5150 c/5150 d, and intermediate tail 5160 a/5160 b/5160 c/5160 d including a shared ground trace, and a proximal electrode pad 5170 a/5170 b/5170 c/5170 d.

In one example, the impedance may be measured at the bipolar electrode pair on proximal electrode pad 5170 b. The measured impedance MZ₁ at proximal electrode pair 5170 b may represent the impedance between the bipolar electrodes of proximal electrode pad 5170 b (e.g., impedance Z₁) along with the impedance between the bipolar electrodes of proximal electrode pad 5170 b and distal electrode pad 5150 b (e.g., impedance Z₁₂), the impedance between the bipolar electrodes of proximal electrode pad 5170 b and proximal electrode pad 5170 b on the opposite side of the balloon (e.g., impedance Z₁₃), and the impedance between the bipolar electrodes of proximal electrode pad 5170 b and distal electrode pad 5150 d on the opposite side of the balloon (e.g., impedance Z₁₄). Because these impedances may be in parallel, the measured impedance MZ₁ may be represented by equation (7):

(1/MZ ₁)=1/Z ₁+1/Z ₁₂+1/Z ₁₃+1/Z ₁₄  Equation (7)

For each of the potential leakage pathways, it has been determined that the impedances Z₁₂, Z₁₃, and Z₁₄ may be related to (i.e. proportional to) the measured impedances MZ₂, MZ₃, and MZ₄, respectively, measured at the corresponding electrode pads 5150 b, 5170 b, 5150 d, according to the following equations:

Z ₁₂ =k ₁₂ MZ ₂  Equation (8)

Z ₁₃ =k ₁₃ MZ ₃  Equation (9)

Z ₁₄ =k ₁₄ MZ ₄  Equation (10)

-   -   where each of k₁₂, k₁₃, and k₁₄ are constants, and where:     -   MZ₂ is the measured impedance at distal electrode pad 5150 b;     -   MZ₃ is the measured impedance at proximal electrode pad 5170 d;         and     -   MZ₄ is the measured impedance at distal electrode pad 5150 d.         These relationships can be substituted into equation (7) and         solved for Z₁ as follows

Z ₁=(MZ₁)(k ₁₂ MZ ₂)(k ₁₃ MZ ₃)(k ₁₄ MZ ₄)/[(k ₁₂ MZ ₂)(k ₁₃ MZ ₃)(k ₁₄ MZ ₄)−(MZ ₁)(k ₁₃ MZ ₃)(k ₁₄ MZ ₄)−(MZ ₁)(k ₁₂ MZ ₂)(k ₁₄ MZ ₄)−(MZ ₁)(k ₁₂ MZ ₂)(k ₁₃ MZ ₃)]  Equation (11)

As can be seen, the measured impedance MZ₁ may be compensated using this linear equation to give a better approximation of the actual impedance Z₁ between the bipolar electrodes on proximal electrode pad 5170 b. While a linear function is shown here, it is contemplated that a non-linear function may be used. In some instance, the linear and/or non-linear function may also be a function of temperature, voltage signals applied to obtain the impedance measurements MZ₁, MZ₂, MZ₃, MZ₄ and/or any other suitable parameter as desired.

Solving equation (11) can be accomplished when the values of k₁₂, k₁₃, and k₁₄ are known. In an example medical device having an outer diameter of 6-7 mm, the value of k₁₂, k₁₃, and k₁₄ have been determined experimentally. For example, k₁₂ may be in the range of about 2.5-4.5, or about 3-4, or about 3.5; k₁₃ may be in the range of about 4.0-6.0, or about 4.5-5.5, or about 5.0; and k₁₄ may be in the range of about 5-7, or about 5.5-6.5, or about 6.0. Accordingly, these values may be utilized to solve for Z₁ in equation (11).

U.S. patent application Ser. No. 13/725,872, filed Dec. 21, 2012; U.S. patent application Ser. No. 13/750,879, filed Jan. 25, 2013; U.S. patent application Ser. No. 13/725,843, filed Dec. 21, 2012; U.S. patent application Ser. No. 13/725,885, filed Dec. 21, 2012; U.S. patent application Ser. No. 13/725,894, filed Dec. 21, 2012; and U.S. patent application Ser. No. 13/725,904, filed Dec. 21, 2012 are all herein incorporated by reference.

While the exemplary embodiments have been described in some detail, by way of example and for clarity of understanding, those of skill in the art will recognize that a variety of modifications, adaptations, and changes may be employed. 

What is claimed is:
 1. A control unit for determining an electrical leakage between a first electrode pad and a second electrode pad of an in vivo medical device, wherein the first electrode pad is spaced from the second electrode pad, and wherein the first electrode pad has an active electrode and a spaced ground electrode, and the second electrode pad has an active electrode and a ground electrode, wherein the ground electrode of the first electrode pad is electrically connected to the ground electrode of the second electrode pad, the control unit comprising: an input/output block for electrically connecting the control unit to the in vivo medical device; a controller communicatively coupled to the input/output block, the controller programmed to: apply a first signal via the input/output block to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad; apply a second signal via the input/output block to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad; and using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.
 2. The control unit of claim 1, wherein the controller is further programmed to compensate the measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad based on the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.
 3. The control unit of claim 1, wherein: the first electrode pad has two or more active electrodes connected together with a first active electrode trace and two or more spaced ground electrodes connected together with a first ground electrode trace; the second electrode pad has two or more active electrodes connected together with a second active electrode trace and two or more spaced ground electrodes connected together with a second ground electrode trace; wherein the first ground electrode trace is electrically connected to the second ground electrode trace forming a common ground electrode trace; and wherein the input/output block of the control unit electrically connects the control unit to the first active electrode trace, the second active electrode trace and the common ground electrode trace.
 4. The control unit of claim 1, wherein the in vivo medical device further includes a third electrode pad that is spaced from the first electrode pad and the second electrode pad, and wherein the third electrode pad has an active electrode and a spaced ground electrode, wherein the ground electrode of the third electrode pad is electrically connected to the ground electrode of the first electrode pad and the second electrode pad, the controller of the control unit further programmed to: apply a third signal via the input/output block to the active electrode of the third electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the third electrode pad and the ground electrode of the third electrode pad; and using the measure that is related to the impedance between the active electrode of the third electrode pad and the ground electrode of the third electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the third electrode pad.
 5. The control unit of claim 1, wherein the controller determines the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by multiplying a constant by the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad.
 6. The control unit of claim 5, wherein the constant is determined by empirical data.
 7. The control unit of claim 1, wherein the controller determines the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad in a linear function.
 8. The control unit of claim 1, wherein the controller determines the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad in a non-linear function.
 9. The control unit of claim 8, wherein the non-linear function is dependent on one or more of temperature and voltage of the applied signals.
 10. The control unit of claim 1, wherein the controller is programmed to apply the signal via the input/output block to the active electrode of the first electrode pad of the in vivo medical device before or after applying the signal via the input/output block to the active electrode of the second electrode pad of the in vivo medical device.
 11. The control unit of claim 1, wherein the controller is programmed to apply the signal via the input/output block to the active electrode of the first electrode pad of the in vivo medical device at the same time as applying the signal via the input/output block to the active electrode of the second electrode pad of the in vivo medical device.
 12. A method for determining an electrical leakage between a first electrode pad and a second electrode pad of an in vivo medical device, wherein the first electrode pad is spaced from the second electrode pad, and wherein the first electrode pad has an active electrode and a spaced ground electrode, and the second electrode pad has an active electrode and a ground electrode, wherein the ground electrode of the first electrode pad is electrically connected to the ground electrode of the second electrode pad, the method comprising: apply a first signal to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad; apply a second signal to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad; using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad; and compensating the measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad based on the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.
 13. The method of claim 12, wherein the first signal is applied before or after the second signal.
 14. The method of claim 12, wherein the first signal is applied at the same time as the second signal.
 15. A system comprising: an in vivo medical device having a first electrode pad and a second electrode pad, wherein the first electrode pad is spaced from the second electrode pad, and wherein the first electrode pad has an active electrode and a spaced ground electrode, and the second electrode pad has an active electrode and a ground electrode, wherein the ground electrode of the first electrode pad is electrically connected to the ground electrode of the second electrode pad; a control unit coupled to the in vivo medical device, the control unit programmed to: apply a first signal to the active electrode of the first electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad; apply a second signal to the active electrode of the second electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad; using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad; and compensating the measure that is related to an impedance between the active electrode of the first electrode pad and the ground electrode of the first electrode pad based on the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad.
 16. The system of claim 15, wherein: the first electrode pad of the in vivo medical device has two or more active electrodes connected together with a first active electrode trace and two or more spaced ground electrodes connected together with a first ground electrode trace; the second electrode pad of in vivo medical device has two or more active electrodes connected together with a second active electrode trace and two or more spaced ground electrodes connected together with a second ground electrode trace; wherein the first ground electrode trace is electrically connected to the second ground electrode trace forming a common ground electrode trace; and wherein the control unit is electrically connected to the first active electrode trace, the second active electrode trace and the common ground electrode trace.
 17. The system of claim 15, wherein the in vivo medical device further includes a third electrode pad that is spaced from the first electrode pad and the second electrode pad, and wherein the third electrode pad has an active electrode and a spaced ground electrode, wherein the ground electrode of the third electrode pad is electrically connected to the ground electrode of the first electrode pad and the second electrode pad, the control unit further programmed to: apply a third signal to the active electrode of the third electrode pad of the in vivo medical device, and in response, determine a measure that is related to an impedance between the active electrode of the third electrode pad and the ground electrode of the third electrode pad; and using the measure that is related to the impedance between the active electrode of the third electrode pad and the ground electrode of the third electrode pad to determine an estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the third electrode pad.
 18. The system of claim 15 wherein the control unit is programmed to determine the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by multiplying a constant by the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad.
 19. The system of claim 15, wherein the control unit determines the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad in a linear function.
 20. The system of claim 15, wherein the controller determines the estimate of the electrical leakage between the active electrode of the first electrode pad and the ground electrode of the second electrode pad by using the measure that is related to the impedance between the active electrode of the second electrode pad and the ground electrode of the second electrode pad in a non-linear function. 